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Vapochromic Coordination Polymer Immobilization Techniques for Ammonia Sensors with Applications
to Power Transformers
by
David Stevens
BASc Simon Fraser University 2015
Thesis Submitted in Partial Fulfillment of the
Requirements for the Degree of
Master of Applied Sciences
in the
School of Engineering Science
Faculty of Applied Science
copy David Stevens 2019
SIMON FRASER UNIVERSITY
Spring 2019
Copyright in this work rests with the author Please ensure that any reproduction or re-use is done in accordance with the relevant national copyright legislation
ii
Approval
Name David Stevens Degree Master of Applied Science (Engineering Science) Title Vapochromic Coordination Polymer Immobilization
Techniques for Ammonia Sensors with Applications to Power Transformers
Examining Committee Chair Michael Sjoerdsma Senior Lecturer
Bonnie Gray Senior Supervisor Professor
Daniel Leznoff Supervisor Professor
Glenn Chapman Internal Examiner Professor
Date DefendedApproved April 16 2019
iii
Abstract
Ammonia detection is important for many applications in the biomedicine
agriculture and automotive industries Sensing of ammonia is also crucial in determining
the health of power transformers as the presence of ammonia indicates a breakdown in
a transformerrsquos insulating materials Current methods of gas analysis for detecting
ammonia in such applications are costly complicated and time consuming This thesis
is concerned with the use of vapochromic coordination polymers (VCPs) which are in
this case fluorescence-based gas sensitive polymers whose emission spectrum
changes upon the binding of target gases eg ammonia VCP materials have shown
great promise in ammonia detection due to their superior fluorescence response and
selectivity to ammonia but require immobilization to enable their use as a sensor
surface The work presented in this thesis examines several different immobilization
techniques for VCPs to create a new class of ammonia sensors
The first immobilization technique explored involves creating a sheet of post
arrays in polydimethylsiloxane (PDMS) to trap and adhere the VCPs to the sensing
surface We show that as the shape of the top of the post arrays is changed (eg from
simple post to mushroom-shaped caps) the sensitivity of the sensing surface changes
Ammonia detection in the amount of 5 ppm is possible with the most pronounced
mushroom shaped posts The second immobilization method involves dissolved
polylactic acid (PLA) mixed with VCPs that are deposited on a PLA substrate resulting
in nanoporous membranes (NPMs) that immobilize the VCP This technique results in
ammonia detection of 5 ppm based on available gas concentrations and reveals that a
mix ratio of PLA to VCP of 12 wt to 88 wt results in a sensor surface with the
highest degree of reversibility This second immobilization technique also makes a
sensor surface that is able to directly detect ammonia dissolved in fluids Because of the
ability of multi-phase gas detection with this immobilization technique we determine that
it is the more promising of the two immobilization methods We explore the application of
both immobilization methods in the creation of a sealed micro-fluidic ammonia sensor
Our prototypes use a 3D printed cyclic olefin copolymer (COC) micro-fluidic cell where
COC is employed due to its exceptional optical properties and chemical inertness These
sensor cells detect ammonia both in gas and dissolved in fluids (transformer oil) but are
limited in a detection of 1000 ppm using available gas concentrations for testing
iv
Keywords power transformers ammonia sensors vapochromic coordination
polymers chemical sensors
v
Acknowledgements
I would like to thank my supervisors Prof B L Gray and Prof D B Leznoff for
their support and freedom to they gave me to work I credit my success to their advice
and assistance throughout the work on this project
Thanks go out to David Yin Prof Glenn Chapman Michael Sjoerdsma all my
lab mates in the engineering and chemistry departments and friends
Without the support of my wife parents and family I would not be able to be
where I am today
vi
Table of Contents
Approval ii Abstractiii Acknowledgements v Table of Contents vi List of Tables viii List of Figures ix List of AbbreviationsGlossary xi
Chapter 1 Introduction 1 11 Overall Contributions of the Thesis 3
Chapter 2 Vapochromic Coordination Polymers 4 21 VCP Synthesis 4 22 Previous work immobilizing VCPs 6 23 Summary 7
Chapter 3 Post Arrays 8 31 Design considerations 8 32 Fabrication 8 33 Fabrication results 10 34 Experimental Methods for Ammonia Detection 13 35 Optical results 14 36 Discussion and summary 23
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM) 24 41 Fabrication of nanoporous membranes (NPMs) 24 42 Fabrication results 25 43 Experimental methods 27 44 Optical results 27 45 Discussion and summary 31
Chapter 5 3D printed ammonia sensor 32 51 Fabrication 32 52 Fabrication results 34 53 Experimental methods 36 54 Optical results 37 55 Discussion and summary 39
Chapter 6 Conclusions and Future work 41 61 Future work 44
611 Post Arrays 44 612 PLA-NPMs and 3D printed fluidic cells 44
References 46
vii
Appendix 49 Fluorescence spectrum data 49
viii
List of Tables
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 16
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle 19
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
21 Table 4 Response comparison between simple post array and mushroom capped post
arrays to 5 ppm NH3 22 Table 5 Pore count size and area of NPM 25 Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace
of 28 NH4OH bottle 29 Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3 30 Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace
of 28 NH4OH bottle 38 Table 9 Comparison of immobilization techniques N2 used as balance gas instead of
air 41
ix
List of Figures
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs 5
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs 6 Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate 7 Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin
coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array This figure has been adapted from material presented in [15] 9
Figure 5 Simple post array without mushroom capped posts 11 Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped
posts 11 Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2 12 Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure
dose of 250 mJcm2 12 Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in
preparation] 13 Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace
of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn
from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from
headspace of 28 NH4OH bottle 17 Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose)
PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 18 Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm
UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle 18
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 19
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3 21
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3 22
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
ii
Approval
Name David Stevens Degree Master of Applied Science (Engineering Science) Title Vapochromic Coordination Polymer Immobilization
Techniques for Ammonia Sensors with Applications to Power Transformers
Examining Committee Chair Michael Sjoerdsma Senior Lecturer
Bonnie Gray Senior Supervisor Professor
Daniel Leznoff Supervisor Professor
Glenn Chapman Internal Examiner Professor
Date DefendedApproved April 16 2019
iii
Abstract
Ammonia detection is important for many applications in the biomedicine
agriculture and automotive industries Sensing of ammonia is also crucial in determining
the health of power transformers as the presence of ammonia indicates a breakdown in
a transformerrsquos insulating materials Current methods of gas analysis for detecting
ammonia in such applications are costly complicated and time consuming This thesis
is concerned with the use of vapochromic coordination polymers (VCPs) which are in
this case fluorescence-based gas sensitive polymers whose emission spectrum
changes upon the binding of target gases eg ammonia VCP materials have shown
great promise in ammonia detection due to their superior fluorescence response and
selectivity to ammonia but require immobilization to enable their use as a sensor
surface The work presented in this thesis examines several different immobilization
techniques for VCPs to create a new class of ammonia sensors
The first immobilization technique explored involves creating a sheet of post
arrays in polydimethylsiloxane (PDMS) to trap and adhere the VCPs to the sensing
surface We show that as the shape of the top of the post arrays is changed (eg from
simple post to mushroom-shaped caps) the sensitivity of the sensing surface changes
Ammonia detection in the amount of 5 ppm is possible with the most pronounced
mushroom shaped posts The second immobilization method involves dissolved
polylactic acid (PLA) mixed with VCPs that are deposited on a PLA substrate resulting
in nanoporous membranes (NPMs) that immobilize the VCP This technique results in
ammonia detection of 5 ppm based on available gas concentrations and reveals that a
mix ratio of PLA to VCP of 12 wt to 88 wt results in a sensor surface with the
highest degree of reversibility This second immobilization technique also makes a
sensor surface that is able to directly detect ammonia dissolved in fluids Because of the
ability of multi-phase gas detection with this immobilization technique we determine that
it is the more promising of the two immobilization methods We explore the application of
both immobilization methods in the creation of a sealed micro-fluidic ammonia sensor
Our prototypes use a 3D printed cyclic olefin copolymer (COC) micro-fluidic cell where
COC is employed due to its exceptional optical properties and chemical inertness These
sensor cells detect ammonia both in gas and dissolved in fluids (transformer oil) but are
limited in a detection of 1000 ppm using available gas concentrations for testing
iv
Keywords power transformers ammonia sensors vapochromic coordination
polymers chemical sensors
v
Acknowledgements
I would like to thank my supervisors Prof B L Gray and Prof D B Leznoff for
their support and freedom to they gave me to work I credit my success to their advice
and assistance throughout the work on this project
Thanks go out to David Yin Prof Glenn Chapman Michael Sjoerdsma all my
lab mates in the engineering and chemistry departments and friends
Without the support of my wife parents and family I would not be able to be
where I am today
vi
Table of Contents
Approval ii Abstractiii Acknowledgements v Table of Contents vi List of Tables viii List of Figures ix List of AbbreviationsGlossary xi
Chapter 1 Introduction 1 11 Overall Contributions of the Thesis 3
Chapter 2 Vapochromic Coordination Polymers 4 21 VCP Synthesis 4 22 Previous work immobilizing VCPs 6 23 Summary 7
Chapter 3 Post Arrays 8 31 Design considerations 8 32 Fabrication 8 33 Fabrication results 10 34 Experimental Methods for Ammonia Detection 13 35 Optical results 14 36 Discussion and summary 23
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM) 24 41 Fabrication of nanoporous membranes (NPMs) 24 42 Fabrication results 25 43 Experimental methods 27 44 Optical results 27 45 Discussion and summary 31
Chapter 5 3D printed ammonia sensor 32 51 Fabrication 32 52 Fabrication results 34 53 Experimental methods 36 54 Optical results 37 55 Discussion and summary 39
Chapter 6 Conclusions and Future work 41 61 Future work 44
611 Post Arrays 44 612 PLA-NPMs and 3D printed fluidic cells 44
References 46
vii
Appendix 49 Fluorescence spectrum data 49
viii
List of Tables
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 16
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle 19
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
21 Table 4 Response comparison between simple post array and mushroom capped post
arrays to 5 ppm NH3 22 Table 5 Pore count size and area of NPM 25 Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace
of 28 NH4OH bottle 29 Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3 30 Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace
of 28 NH4OH bottle 38 Table 9 Comparison of immobilization techniques N2 used as balance gas instead of
air 41
ix
List of Figures
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs 5
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs 6 Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate 7 Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin
coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array This figure has been adapted from material presented in [15] 9
Figure 5 Simple post array without mushroom capped posts 11 Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped
posts 11 Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2 12 Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure
dose of 250 mJcm2 12 Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in
preparation] 13 Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace
of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn
from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from
headspace of 28 NH4OH bottle 17 Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose)
PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 18 Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm
UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle 18
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 19
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3 21
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3 22
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
iii
Abstract
Ammonia detection is important for many applications in the biomedicine
agriculture and automotive industries Sensing of ammonia is also crucial in determining
the health of power transformers as the presence of ammonia indicates a breakdown in
a transformerrsquos insulating materials Current methods of gas analysis for detecting
ammonia in such applications are costly complicated and time consuming This thesis
is concerned with the use of vapochromic coordination polymers (VCPs) which are in
this case fluorescence-based gas sensitive polymers whose emission spectrum
changes upon the binding of target gases eg ammonia VCP materials have shown
great promise in ammonia detection due to their superior fluorescence response and
selectivity to ammonia but require immobilization to enable their use as a sensor
surface The work presented in this thesis examines several different immobilization
techniques for VCPs to create a new class of ammonia sensors
The first immobilization technique explored involves creating a sheet of post
arrays in polydimethylsiloxane (PDMS) to trap and adhere the VCPs to the sensing
surface We show that as the shape of the top of the post arrays is changed (eg from
simple post to mushroom-shaped caps) the sensitivity of the sensing surface changes
Ammonia detection in the amount of 5 ppm is possible with the most pronounced
mushroom shaped posts The second immobilization method involves dissolved
polylactic acid (PLA) mixed with VCPs that are deposited on a PLA substrate resulting
in nanoporous membranes (NPMs) that immobilize the VCP This technique results in
ammonia detection of 5 ppm based on available gas concentrations and reveals that a
mix ratio of PLA to VCP of 12 wt to 88 wt results in a sensor surface with the
highest degree of reversibility This second immobilization technique also makes a
sensor surface that is able to directly detect ammonia dissolved in fluids Because of the
ability of multi-phase gas detection with this immobilization technique we determine that
it is the more promising of the two immobilization methods We explore the application of
both immobilization methods in the creation of a sealed micro-fluidic ammonia sensor
Our prototypes use a 3D printed cyclic olefin copolymer (COC) micro-fluidic cell where
COC is employed due to its exceptional optical properties and chemical inertness These
sensor cells detect ammonia both in gas and dissolved in fluids (transformer oil) but are
limited in a detection of 1000 ppm using available gas concentrations for testing
iv
Keywords power transformers ammonia sensors vapochromic coordination
polymers chemical sensors
v
Acknowledgements
I would like to thank my supervisors Prof B L Gray and Prof D B Leznoff for
their support and freedom to they gave me to work I credit my success to their advice
and assistance throughout the work on this project
Thanks go out to David Yin Prof Glenn Chapman Michael Sjoerdsma all my
lab mates in the engineering and chemistry departments and friends
Without the support of my wife parents and family I would not be able to be
where I am today
vi
Table of Contents
Approval ii Abstractiii Acknowledgements v Table of Contents vi List of Tables viii List of Figures ix List of AbbreviationsGlossary xi
Chapter 1 Introduction 1 11 Overall Contributions of the Thesis 3
Chapter 2 Vapochromic Coordination Polymers 4 21 VCP Synthesis 4 22 Previous work immobilizing VCPs 6 23 Summary 7
Chapter 3 Post Arrays 8 31 Design considerations 8 32 Fabrication 8 33 Fabrication results 10 34 Experimental Methods for Ammonia Detection 13 35 Optical results 14 36 Discussion and summary 23
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM) 24 41 Fabrication of nanoporous membranes (NPMs) 24 42 Fabrication results 25 43 Experimental methods 27 44 Optical results 27 45 Discussion and summary 31
Chapter 5 3D printed ammonia sensor 32 51 Fabrication 32 52 Fabrication results 34 53 Experimental methods 36 54 Optical results 37 55 Discussion and summary 39
Chapter 6 Conclusions and Future work 41 61 Future work 44
611 Post Arrays 44 612 PLA-NPMs and 3D printed fluidic cells 44
References 46
vii
Appendix 49 Fluorescence spectrum data 49
viii
List of Tables
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 16
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle 19
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
21 Table 4 Response comparison between simple post array and mushroom capped post
arrays to 5 ppm NH3 22 Table 5 Pore count size and area of NPM 25 Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace
of 28 NH4OH bottle 29 Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3 30 Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace
of 28 NH4OH bottle 38 Table 9 Comparison of immobilization techniques N2 used as balance gas instead of
air 41
ix
List of Figures
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs 5
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs 6 Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate 7 Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin
coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array This figure has been adapted from material presented in [15] 9
Figure 5 Simple post array without mushroom capped posts 11 Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped
posts 11 Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2 12 Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure
dose of 250 mJcm2 12 Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in
preparation] 13 Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace
of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn
from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from
headspace of 28 NH4OH bottle 17 Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose)
PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 18 Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm
UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle 18
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 19
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3 21
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3 22
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
iv
Keywords power transformers ammonia sensors vapochromic coordination
polymers chemical sensors
v
Acknowledgements
I would like to thank my supervisors Prof B L Gray and Prof D B Leznoff for
their support and freedom to they gave me to work I credit my success to their advice
and assistance throughout the work on this project
Thanks go out to David Yin Prof Glenn Chapman Michael Sjoerdsma all my
lab mates in the engineering and chemistry departments and friends
Without the support of my wife parents and family I would not be able to be
where I am today
vi
Table of Contents
Approval ii Abstractiii Acknowledgements v Table of Contents vi List of Tables viii List of Figures ix List of AbbreviationsGlossary xi
Chapter 1 Introduction 1 11 Overall Contributions of the Thesis 3
Chapter 2 Vapochromic Coordination Polymers 4 21 VCP Synthesis 4 22 Previous work immobilizing VCPs 6 23 Summary 7
Chapter 3 Post Arrays 8 31 Design considerations 8 32 Fabrication 8 33 Fabrication results 10 34 Experimental Methods for Ammonia Detection 13 35 Optical results 14 36 Discussion and summary 23
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM) 24 41 Fabrication of nanoporous membranes (NPMs) 24 42 Fabrication results 25 43 Experimental methods 27 44 Optical results 27 45 Discussion and summary 31
Chapter 5 3D printed ammonia sensor 32 51 Fabrication 32 52 Fabrication results 34 53 Experimental methods 36 54 Optical results 37 55 Discussion and summary 39
Chapter 6 Conclusions and Future work 41 61 Future work 44
611 Post Arrays 44 612 PLA-NPMs and 3D printed fluidic cells 44
References 46
vii
Appendix 49 Fluorescence spectrum data 49
viii
List of Tables
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 16
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle 19
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
21 Table 4 Response comparison between simple post array and mushroom capped post
arrays to 5 ppm NH3 22 Table 5 Pore count size and area of NPM 25 Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace
of 28 NH4OH bottle 29 Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3 30 Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace
of 28 NH4OH bottle 38 Table 9 Comparison of immobilization techniques N2 used as balance gas instead of
air 41
ix
List of Figures
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs 5
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs 6 Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate 7 Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin
coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array This figure has been adapted from material presented in [15] 9
Figure 5 Simple post array without mushroom capped posts 11 Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped
posts 11 Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2 12 Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure
dose of 250 mJcm2 12 Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in
preparation] 13 Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace
of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn
from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from
headspace of 28 NH4OH bottle 17 Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose)
PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 18 Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm
UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle 18
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 19
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3 21
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3 22
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
v
Acknowledgements
I would like to thank my supervisors Prof B L Gray and Prof D B Leznoff for
their support and freedom to they gave me to work I credit my success to their advice
and assistance throughout the work on this project
Thanks go out to David Yin Prof Glenn Chapman Michael Sjoerdsma all my
lab mates in the engineering and chemistry departments and friends
Without the support of my wife parents and family I would not be able to be
where I am today
vi
Table of Contents
Approval ii Abstractiii Acknowledgements v Table of Contents vi List of Tables viii List of Figures ix List of AbbreviationsGlossary xi
Chapter 1 Introduction 1 11 Overall Contributions of the Thesis 3
Chapter 2 Vapochromic Coordination Polymers 4 21 VCP Synthesis 4 22 Previous work immobilizing VCPs 6 23 Summary 7
Chapter 3 Post Arrays 8 31 Design considerations 8 32 Fabrication 8 33 Fabrication results 10 34 Experimental Methods for Ammonia Detection 13 35 Optical results 14 36 Discussion and summary 23
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM) 24 41 Fabrication of nanoporous membranes (NPMs) 24 42 Fabrication results 25 43 Experimental methods 27 44 Optical results 27 45 Discussion and summary 31
Chapter 5 3D printed ammonia sensor 32 51 Fabrication 32 52 Fabrication results 34 53 Experimental methods 36 54 Optical results 37 55 Discussion and summary 39
Chapter 6 Conclusions and Future work 41 61 Future work 44
611 Post Arrays 44 612 PLA-NPMs and 3D printed fluidic cells 44
References 46
vii
Appendix 49 Fluorescence spectrum data 49
viii
List of Tables
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 16
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle 19
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
21 Table 4 Response comparison between simple post array and mushroom capped post
arrays to 5 ppm NH3 22 Table 5 Pore count size and area of NPM 25 Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace
of 28 NH4OH bottle 29 Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3 30 Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace
of 28 NH4OH bottle 38 Table 9 Comparison of immobilization techniques N2 used as balance gas instead of
air 41
ix
List of Figures
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs 5
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs 6 Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate 7 Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin
coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array This figure has been adapted from material presented in [15] 9
Figure 5 Simple post array without mushroom capped posts 11 Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped
posts 11 Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2 12 Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure
dose of 250 mJcm2 12 Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in
preparation] 13 Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace
of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn
from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from
headspace of 28 NH4OH bottle 17 Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose)
PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 18 Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm
UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle 18
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 19
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3 21
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3 22
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
vi
Table of Contents
Approval ii Abstractiii Acknowledgements v Table of Contents vi List of Tables viii List of Figures ix List of AbbreviationsGlossary xi
Chapter 1 Introduction 1 11 Overall Contributions of the Thesis 3
Chapter 2 Vapochromic Coordination Polymers 4 21 VCP Synthesis 4 22 Previous work immobilizing VCPs 6 23 Summary 7
Chapter 3 Post Arrays 8 31 Design considerations 8 32 Fabrication 8 33 Fabrication results 10 34 Experimental Methods for Ammonia Detection 13 35 Optical results 14 36 Discussion and summary 23
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM) 24 41 Fabrication of nanoporous membranes (NPMs) 24 42 Fabrication results 25 43 Experimental methods 27 44 Optical results 27 45 Discussion and summary 31
Chapter 5 3D printed ammonia sensor 32 51 Fabrication 32 52 Fabrication results 34 53 Experimental methods 36 54 Optical results 37 55 Discussion and summary 39
Chapter 6 Conclusions and Future work 41 61 Future work 44
611 Post Arrays 44 612 PLA-NPMs and 3D printed fluidic cells 44
References 46
vii
Appendix 49 Fluorescence spectrum data 49
viii
List of Tables
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 16
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle 19
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
21 Table 4 Response comparison between simple post array and mushroom capped post
arrays to 5 ppm NH3 22 Table 5 Pore count size and area of NPM 25 Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace
of 28 NH4OH bottle 29 Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3 30 Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace
of 28 NH4OH bottle 38 Table 9 Comparison of immobilization techniques N2 used as balance gas instead of
air 41
ix
List of Figures
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs 5
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs 6 Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate 7 Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin
coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array This figure has been adapted from material presented in [15] 9
Figure 5 Simple post array without mushroom capped posts 11 Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped
posts 11 Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2 12 Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure
dose of 250 mJcm2 12 Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in
preparation] 13 Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace
of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn
from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from
headspace of 28 NH4OH bottle 17 Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose)
PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 18 Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm
UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle 18
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 19
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3 21
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3 22
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
vii
Appendix 49 Fluorescence spectrum data 49
viii
List of Tables
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 16
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle 19
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
21 Table 4 Response comparison between simple post array and mushroom capped post
arrays to 5 ppm NH3 22 Table 5 Pore count size and area of NPM 25 Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace
of 28 NH4OH bottle 29 Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3 30 Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace
of 28 NH4OH bottle 38 Table 9 Comparison of immobilization techniques N2 used as balance gas instead of
air 41
ix
List of Figures
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs 5
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs 6 Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate 7 Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin
coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array This figure has been adapted from material presented in [15] 9
Figure 5 Simple post array without mushroom capped posts 11 Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped
posts 11 Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2 12 Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure
dose of 250 mJcm2 12 Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in
preparation] 13 Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace
of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn
from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from
headspace of 28 NH4OH bottle 17 Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose)
PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 18 Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm
UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle 18
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 19
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3 21
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3 22
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
viii
List of Tables
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 16
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle 19
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
21 Table 4 Response comparison between simple post array and mushroom capped post
arrays to 5 ppm NH3 22 Table 5 Pore count size and area of NPM 25 Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace
of 28 NH4OH bottle 29 Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3 30 Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace
of 28 NH4OH bottle 38 Table 9 Comparison of immobilization techniques N2 used as balance gas instead of
air 41
ix
List of Figures
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs 5
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs 6 Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate 7 Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin
coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array This figure has been adapted from material presented in [15] 9
Figure 5 Simple post array without mushroom capped posts 11 Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped
posts 11 Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2 12 Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure
dose of 250 mJcm2 12 Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in
preparation] 13 Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace
of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn
from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from
headspace of 28 NH4OH bottle 17 Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose)
PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 18 Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm
UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle 18
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 19
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3 21
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3 22
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
ix
List of Figures
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs 5
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs 6 Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate 7 Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin
coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array This figure has been adapted from material presented in [15] 9
Figure 5 Simple post array without mushroom capped posts 11 Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped
posts 11 Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2 12 Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure
dose of 250 mJcm2 12 Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in
preparation] 13 Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace
of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn
from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors 15 Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from
headspace of 28 NH4OH bottle 17 Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose)
PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 18 Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm
UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle 18
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle 19
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3 20
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3 21
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3 22
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
x
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey) 26
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey) 26 Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3
drawn from headspace of 28 NH4OH bottle 28 Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to
NH3drawn from headspace of 28 NH4OH bottle 28 Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5
ppm NH3 30 Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5
ppm NH3 31 Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell 33 Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-
Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs 34
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals 35
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals) 36
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 37
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell 38
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF 39
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light 40 Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-
NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 49
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 49
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 50
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 50
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics) 51
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics) 51
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
xi
List of AbbreviationsGlossary
COC Cyclic olefin copolymer
COC-NF Cyclic olefin copolymer ndash nanofiber
C6H12 Cyclohexane
DCM Dichloromethane
DGA Differential Gas Analysis
GC Gas Chromatography
NH3 Ammonia
NPM Nanoporous Membrane
PDMS Polydimethylsiloxane
PLA Poly(lactic) Acid
PLA-NPM Poly(lactic) Acid ndash Nanoporous Membrane
PMGI Polymethylglutarimide
PPM Parts per million
THF Tetrahydrofuran
VCP Vapochromic Coordination Polymer
VOC Volatile Organic Compound
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
1
Chapter 1 Introduction
Power transformers are one of the single most expensive and critical
components of todayrsquos power systems Their failures cause significant losses and risks
in terms of power outages explosions fires and loss of life and property The early
detection of potential failures can mitigate these losses and risks The most common
method currently used to detect potential failures is through the use of gas
chromatography (GC) and diffused gas analysis (DGA) Transformer oil which acts as an
insulator is extracted by an operator from the power transformer for analysis in a
laboratory which may be a long distance from where the oil sample was taken from
DGA uses different methods (ie Doernenburg Ratio [1] and Duval Triangles [2]) to
determine what gasses are present in the power transformer oil GC on the other hand
separates volatile organic compounds (VOCs) based on their relative affinities for
different phases The type of gas and relative quantity in relation to others can indicate
the severity and type of fault that has occurred within the power transformer A key
breakdown gas of interest is ammonia Ammonia is a breakdown by-product that is
released from the insulation when certain faults such as arcing partial discharge and
overheating cause the insulation around the coils to breakdown
As an alternative to using GC or DGA for the detection of ammonia many new
types of gas sensors have been developed to address the need of detecting ammonia
for many different applications Such sensors can be generally divided into different
categories such as metal oxide [2 3] catalytic [4 5] conductive polymer [6 7 8] and
optical sensing [9 10] Metal oxide sensors for example are both inexpensive and
capable of detecting ammonia at levels of 1 ppm and below However both their lack of
selectivity and high operating temperatures make them unsuitable for ammonia
detection in a power transformer environment While there has been good progress on
the development of many of the other types of ammonia sensors they have generally
been targeted for applications whose operating condition and requirements are likewise
incompatible with the detection of ammonia inside power transformers Similar to DGA
and GC these sensors are primarily limited to gas analysis and cannot directly detect
dissolved gasses
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
2
In order to overcome these limitations sensors based on vapochromic
coordination polymers (VCPs) are under investigation because of their chemical and
thermal stability especially in the presence of water and specific selectivity to the target
gas(es) However while these sensors show promise in terms of ammonia detection
methods to immobilize VPCs on sensor surfaces has proven to be very challenging due
to their intrinsic chemical and thermal stability especially when the sensors intended
applications are also to detect ammonia that is dissolved in oil
The overall goal of this thesis is to develop robust simple and inexpensive
immobilization techniques in order to demonstrate a new class of optical based ammonia
sensors employing VCPs The immobilization techniques should result in sensors that
may be used in the field for detection of low concentrations of the level of 1 ppm for
applications including but potentially not limited to the monitoring of power transformer
health The VCP Zn[Au(CN)2]2 is a fluorescence-based gas sensitive polymer whose
emission spectrum changes upon the binding of ammonia Its physical and chemical
nature makes it very robust but also very difficult to immobilize due to the inability of the
VCPs to dissolve in solvents to allow them to make thin films or easily combined with
other materials Other researchers working on the project have attempted to brominate it
to make it into a thin film to give the VCP the required high surface area to volume ratios
required to be most effective This thesis instead proposes physical entrapment methods
that are simple repeatable and low cost to achieve the same requirement
The first immobilization method involves creating post arrays in
polydimethylsiloxane (PDMS) based on the concept of biomimetic dry adhesives [15]
The geometries and morphology of the post arrays provide a good environment for the
physical entrapment of the VCP crystals while ensuring that gas can freely move within
the post arrays and fully access the VCPs The second immobilization method involves
creating nanoporous membranes (NPMs) from polylactic acid (PLA) The gasfluid
breathable membranes that entrap the VCPs provide long-term physical immobilization
that allows for a sensing surface that can be used to detect ammonia in gasses as well
as ammonia dissolved in fluids Both immobilization methods are tested and contrasted
against un-immobilized VCP in bulk form through the use of the optical detection
methods developed by Yin et al [19] Lastly a 3D printed cyclic olefin copolymer (COC)
micro fluidic cell is made to test the immobilization methods for ammonia gas and as
dissolved in liquid
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
3
The organization of the thesis is as follows Chapter 2 introduces the background
of the class of VCPs discussed in this thesis Chapter 3 introduces the first
immobilization technique including design fabrication test setup and results Chapter 4
discusses the process of the second immobilization technique test setup and results
Chapter 5 introduces the 3D printed micro fluidic cell and explores the importance of the
VCP synthesis and morphology and its effects on immobilization Chapter 6 presents
comparative results of the work presented in this thesis conclusions and future work
11 Overall Contributions of the Thesis
This thesis makes the following contributions to the area of VCP immobilization
techniques
bull Development of mushroom capped post arrays for improved physical
immobilization of VCPs resulting in sensors that are capable of 5 ppm of
ammonia detection
bull Development of PLA based nanoporous membranes (NPMs) that provide long-
term physical immobilization good reversibility and multiphase ammonia
detection (eg ammonia as gas or ammonia dissolved in fluids) This technique
results in sensors that detect ammonia at 5 ppm concentrations
bull Development of first-generation new NPMs from COC resulting in the creation of
COC nanofibers (NFs) that immobilize particles
It is noted that initial work with post arrays was published and presented at the
IEEE Sensors 2017 conference [18] The other results remain as yet unpublished
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
4
Chapter 2 Vapochromic Coordination Polymers
Vapochromic coordination polymers (VCPs) are a class of compounds used as
the optical equivalent of electronic noses in the detection of volatile organic compounds
(VOCs) Vapochromic compounds are compounds with an emission spectrum or color
that shifts in the presence of a target VOC The VCPs under study in this thesis undergo
a fluorescence emission spectrum shift in the presence of ammonia (NH3) The VCPs
that we explore here are also reversible (ie when gas is released emission spectrum
returns to original state) which is a key requirement for sensors and the VCPs
reversibility is positively temperature dependent
VCPs are attractive for use in VOC sensing eg ammonia sensors because of
their potential for miniaturization selectivity to ammonia and chemical and thermal
stability Additionally VCPs are attractive due to the potential to directly detect ammonia
that is dissolved in fluids allowing greater versatility in the potential sensing
environments However a major drawback due to their robust chemical and thermal
stability makes them hard to immobilize due to the fact that they cannot readily be
dissolved in solvents and manipulated
21 VCP Synthesis
The main VCP that is used in the work presented in this thesis is Zn[Au(CN)2]2 of
which there are four polymorphs (α β γ δ) that can be formed from various methods of
synthesis However after complete or saturated exposure to ammonia and the
subsequent release of ammonia from the VCP crystals all polymorphs revert to the α
polymorph The polymorphs featured in this thesis are a and b because of the relative
ease of synthesis of these two polymorphs and the subsequent reversion to the α
polymorph These two polymorphs also represent the two main physical crystal structure
morphologies hexagonal and sheet shaped or a and b respectively The two
polymorphs α-Zn[Au(CN)2]2 and b-Zn[Au(CN)2]2 are synthesized using the processes
outlined by Katz et al [12] or Hoskins et al [13] Sample formulations for the synthesis of
both α and β polymorphs are shown in equations 1 and 2 The synthesized VCP
particles have sizes ranging from a few to tens of microns as observed in Figure 1
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
5
2119870119860119906(119862119873)) + 119885119899(119862119897119874))6119867)1198743456789⎯⎯⎯ 120572 minus 119885119899[119860119906(119862119873))]) (1)
119885119899(119873119874A)) + 2[(119899 minus 119861119906)119873][119860119906(119862119873))] 1 2D 119867)1198743456789⎯⎯⎯ 120573 minus 119885119899[119860119906(119862119873))]) (2)
Additionally other VCPs of the composition of Zn[Pt(CN)4] and Cd[Au(CN)2]2 are
also experimented with as it is expected that their behavior in terms of immobilization
should be identical Figure 1 shows pictures of the crystallites of α-Zn[Au(CN)2]2 and β-
Zn[Au(CN)2]2 respectively which shows hexagonal and plate morphology shapes for
each respective polymorph Figure 2 shows the crystallites of Zn[Pt(CN)4] with mixed
polymorphs
Figure 1 SEM image of VCPs α-Zn[Au(CN)2]2 (left) and β- Zn[Au(CN)2]2 (right) polymorphs
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
6
Figure 2 SEM image of Zn[Pt(CN)4] VCP crystallites with mixed polymorphs
22 Previous work immobilizing VCPs
Other researchers work on immobilizing the Zn[Au(CN)2]2 VCP employed
brominating it to form the chemical composition of Zn[AuBr2(CN)2]2 and make it soluble
in ethanol This makes the polymer spin-coat-able on a substrate to improve its
functionality and stability However this process requires an extremely long time to
optically trigger the reductive elimination of the bromine through the use of a frequency
doubled NdYag laser to ensure that the base VCP is regenerated and is able to
fluoresce While continuous wave laser excitation sources of the wavelengths of 345 nm
and 390 nm for the α and β polymorphs respectively are preferential for optimal
excitation a 405 nm laser source is instead chosen because of its high power and
inexpensiveness over the lower wavelength sources
Attempts are made to thermally trigger the reduction of the bromine similar to the
method that was done by Ovens et al [14] However it is discovered through
experimentation that this results in the decomposition of the coordination polymer
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
7
instead of the intended reduction of bromine It is thought that this result is due to the
fact that the brominated Zn[AuBr2(CN)2]2 polymer is not a pyrazine-based system that
exhibited the hydrothermal reduction (eg bromine atoms are ejected from crystal lattice
when heated) [14] Figure 3 shows the thin film crystallization of brominated VCP on a
glass substrate
This previous work on immobilization does create a fluorescing sensor surface as
a thin film with a high surface area to volume ratio The major issue with this previous
immobilization work is that is difficult to reproduce with reliable characteristics and
requires expensive equipment that may not be readily available
Figure 3 Thin film crystal of Zn[AuBr2(CN)2]2 on glass substrate
23 Summary
We have discussed the basics behind VCPs and their appeal as use in the
development of ammonia sensors due to their intrinsic fluorescence nature chemical
and thermal stability and specific selectivity to ammonia gas However we have also
discussed that the only current method of immobilization while effective in gas
detection is also difficult and expensive to perform
The next chapters focus on outlining design considerations and fabrication
processes to immobilize the VCPs into sensor surfaces to address the limitations
presented in this chapter and the current immobilization technique
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
8
Chapter 3 Post Arrays
31 Design considerations
VCPs have optimal performance when a high surface area to volume ratio is
realized and is exposed to gases It is also of great consideration to pick immobilization
materials that will not absorb reflect or fluoresce at the wavelengths that we are trying
to detect at (eg 400 ndash 550 nm) and therefore any physical immobilization methods
require that these criteria be met as best as possible As stated in the previous chapter
existing immobilization methods are lacking For instance the only method that has
been attempted is through the chemical alteration by bromination and the subsequent
removal to create a thin film However that method is costly and time consuming and is
not practical for large scale production of sensors
The biomimetic dry adhesives fabricated in polydimethylsiloxane (PDMS)
demonstrated by Sameoto et al [15] are examined as an alternative to fulfil the criteria of
immobilization while potentially solving problems of gas access to the VCPs The post
arrays have both the physical geometries and morphologies that should support physical
entrapment of the VCP particles while allowing gas access PDMS also does not
optically interfere with the VCPs as determined by initial experimentation with flat PDMS
samples The initial design of post sizes and spacing is chosen because it is shown that
it would create a post array that is proven to be an effective biomimetic dry adhesive [15]
and it is thought that it would be able to accept the VCP crystals within the post array
VCP crystal synthesis results in grain sizes are in the range of a few to 10rsquos of microns
which can be further reduced through the means of hand grinding the crystals with a
mortar and pestle The size range of the VCPs are therefore of the sizes where the
physical entrapment by the posts may be expected to engage to immobilize the VCP
32 Fabrication
The initial design consists of an array of posts where it employs photolithography
and soft lithography [15] for fabricating 10 μm posts spaced 20 μm apart center to
center Figure 4 outlines the micro-fabrication process that is followed to produce the
post arrays presented in this thesis A silicon wafer is coated with 5 nm50 nm
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
9
ChromiumGold (CrAu) to form an adhesion layer for polymethylglutarimide (PMGI)
(supplied by MicroChem Corp Westborough MA) The PMGI layer is a deep UV
sensitive photoresist that allows for undercutting and is designed for lift-off procedures
PMGI SF 19 photoresist is mixed 11 by weight with PMGI T thinner (also from
MicroChem Corp) The PMGI is spun at 500 rpm for 10 seconds followed by 1000 rpm
for 30 seconds It is then soft baked at 100 degC for one minute and then hard baked at
180 degC for three minutes
Figure 4 (a) A silicon wafer is coated with 5nm50 nm CrAu that is followed by spin coating and baking of PMGI and AZ 9260 photoresist (b) The photoresist is exposed to the post array mask (c) Photoresist is
developed and dried leaving undercut areas (d) Slygard 184 is mixed and poured into mold and cured (e) The cured siicone is demolded and inverted producing the post array
Two different designs are considered simple and mushroom capped post arrays
For the fabrication of mushroom capped post arrays an inexpensive 254 nm UV light
source is used (Stratalinker 2400 from Stratagene) The wafer is then exposed to
varying doses between 200 and 300 mJcm2 to increase the development rate of the
PMGI layer which in turn increases the amount of undercutting and therefore increases
the mushroom cap diameter No exposure is done for the simple post arrays After the
wafer is cooled andor exposed to the 254 nm light source AZ 9260 is spin coated at
500 rpm for 10 seconds and then 1000 rpm for 30 seconds The wafer is then left to
relax for 5 minutes and then rehydrated in de-ionized (DI) water for 30 minutes and then
dried with N2 gas The wafer is then exposed to 3 minutes of i-line ultraviolet (365 nm
UV) light at a nominal power of 20 mWcm2 For the simple post arrays where there was
no 254 nm UV exposure of the PMGI the development of the wafer is finished by
immersing it in AZ 400K 14 for 6 minutes Next it is immersed it in MF-319 developer
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
10
for 15 minutes and dried with N2 gas Development times for the mushroom capped
post arrays are varied to compensate for the changes to the rates of development for the
PMGI
Slygard 184 is mixed in a 110 (precursorsilicon) ratio and degassed for 1 hour
It is spun on the wafer at 350 rpm for 30 seconds The coated wafer is then degassed for
1 hour After degassing the wafer is cured on a hotplate at 50 degC for 12 hours and then
hard baked to promote strengthening of the PDMS for another 30 minutes at 120 degC
After the curing process the PDMS layer is demolded by hand from the wafer The
PDMS layer is then imaged by a scanning electron microscope (SEM) to reveal the
resulting post array
The Zn[Au(CN)2]2 VCPs are thoroughly mixed with ethanol to form a uniform
suspension In order to ensure consistency all suspensions are formed using exactly the
same masses of VCP crystals to volumes of ethanol The suspension solutions are
drawn into a syringe and quickly drop cast onto the PDMS post arrays The ethanol is
evaporated at room temperature leaving the VCP immobilized within the post arrays
33 Fabrication results
Figure 5 shows an example of a fabricated simple post array imaged with a
scanning electron microscope (SEM) (Explorer FEIAspex) We see that the posts are
uniform and average around 124 μm in diameter and approximately 194 μm center to
center in spacing which is within 19 and 3 of the design specifications for the posts
and spacing The post heights are approximately 20 μm tall Due to the fact that the
Zn[Au(CN)2]2 VCP is drop cast onto the PDMS post array without any surface treatment
of the post array the VCP does not fully immobilize within the post array (between the
posts) as intended (Figure 6) However we see that the VCP is attached both on the
surface and in spaces between the posts of the array Surface treatments of the
fabricated post surfaces such as oxygen plasma to induce hydrophilicity before VCP
application may help it to penetrate between the posts Also if the distance between the
posts were greater for future experiments the VCP may integrate better The degree of
immobilization that is achieved between the different types of post arrays is not
measured post fabrication other than to note how readily VCPs are ejected via physical
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
11
manipulation The level of immobilization between the different post arrays is inferred by
the optical response results
Figure 5 Simple post array without mushroom capped posts
Figure 6 Immobilized ball milled VCPs in simple post array without mushroom capped posts
As a comparison Figure 7 shows an example of a fabricated mushroom capped
post array that received a 200 mJcm2 dose of 254 nm UV light We see again that the
posts are uniform (some post defects observed) with an average diameter of 145 microm
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
12
Figure 7 Mushroom capped post array ndash PMGI UV exposure dose of 200 mJcm2
In Figure 8 we observe that the average post size increases to 156 microm when
the UV dose is increased to 250 mJcm2 Figure 8 shows VCPs in their original
synthesized form whereas their form after ball milling as observed in Figure 6 While it
appears that there is more uniform coverage with the ball milled VCP crystals in the post
array it is accompanied with what is observed as an overall reduction of VCP in the
same post array area
Figure 8 Mushroom capped post array with immobilized VCPs - PMGI UV exposure dose of 250 mJcm2
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
13
34 Experimental Methods for Ammonia Detection
The VCPs are immobilized on the post arrays and a piece with the dimensions of
1 cm by 05 cm is cut from the post array and put inside a 35 mL cork-sealed quartz
cuvette as shown in Figure 9 A 30 mW 405 nm deep-violet continuous wave diode
laser is used to excite the sample and causes a base emission which peaks at
approximately 480 nm A small spectrometer (PhotonControl SPM-002) records the
digital spectrum which is further computer processed using Matlab The optical results of
ammonia exposure of the samples use two different methods of data analysis in Matlab
The first method involves wavelength and intensity shifts which are clearly discernable at
concentrations of 1000 ppm and greater However for concentrations 1000 ppm and
below a different method of data analysis is needed This method called Spectral Region
Subtraction (SRS) and was developed by Yin et al [19] By tracking the integrated
emission intensities of two spectral regions (unexposed and exposed) their subtracted
difference returns the detection signal
A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle which is thought to result in a gas
concentration of approximately 50000 ppm depending on bottle contents and
temperature at the time of extraction Next 10 mL of this highly concentrated ammonia
gas is then pumped into the cuvette at a rate of approximately 1 mLs
Figure 9 Experimental setup for optical fluorescence detection [D Yin thesis in preparation]
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
14
The experiment is then repeated using un-immobilized VCP attached to a 1 cm
by 05 cm piece of double-sided tape to serve as a baseline comparison It is then also
repeated with VCP on a fully cured flat PDMS surface to show the loss of adhesion that
occurs over time under gas flow The experiment is repeated with VCP in simple and
mushroom capped post arrays for comparisons
Additional experiments are performed using calibrated gas tanks of ammonia
mixed with N2 as the balancing gas for the concentration of 1000 ppm Calibrated gas
tanks of ammonia mixed with lab air as the balancing gas are used to test at
concentrations of 50 ppm and 5 ppm Using the calibrated ammonia tanks the gas is
pumped into the sample cuvette at a rate of 194 mLs
35 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the
immobilization technique and when we compare these results using the post-based
immobilization technique to the response of a sample of un-immobilized VCP in cuvette
little difference is observed Figure 10 shows the fluorescence response for the un-
immobilized VCP while Figure 11 shows the fluorescence response of VCP that is
immobilized on a simple PDMS post array The responses between the samples is very
similar but with the immobilized VCP taking approximately 90 seconds longer to reach
maximum intensity when exposed to ammonia It is thought that the slower response
time is due to increased diffusion time of the ammonia to the VCP within the post array
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
15
Figure 10 Fluorescence response of un-immobilized VCP to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Figure 11 Fluorescence response of VCP on PDMS simple post array to NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Looking at Figure 10 and Figure 11 the initial (unexposed) material peaks at
465 nm in the un-immobilized condition and shows a broad emission By comparison in
the case with VCP immobilized on a post array the initial spectrum is more sharply
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
16
peaked at about 480 nm a shift of about 15 nm The optical response is defined as the
emission peak wavelength shift from its unexposed state as well as its change in
relative intensity The response time is defined as the time required for the peak intensity
to reach 90 of the maximum value Table 1 shows the comparison of the behavior
between the un-immobilized VCP and that immobilized in our post array From Figure 10
and Figure 11 and Table 1 it is seen that the post exposure spectral peak shift is
reduced by about 25 nm in the immobilized sample The relative intensity peak gain is
still large though reduced from 495 (un-immobilized) to 389 (immobilized) but that is
likely because the pre-exposure spectrum is more highly peaked but less spectrally
broad than that of the un-immobilized spectrum
Table 1 Response comparison between un-immobilized and immobilized VCP NH3 drawn from headspace of 28 NH4OH bottle [18] Oacute 2017 IEEE Sensors
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec) (90 of max)
Un-immobilized 478 4949 115
Immobilized 253 3896 70
The actual peak intensity of the exposed material is higher for the immobilized
case In using the VCP to quantitatively measure the ammonia our work has found that
the peak spectral shift is less useful than measuring the intensity of the spectrum at the
peak wavelength Additionally the spectral width and shape is more important in the
analysis of the optical response than the peak spectral shift at lower ammonia
concentrations where there will be little difference between the pre-exposure and full-
exposure peak wavelengths
The fluorescence response is shown as a function of time but that is just to
illustrate that the response is quick the actual interest is the fluorescence response in
steady-state equilibrium and not any time or concentration variations
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
17
Figure 12 Fluorescence response of VCP on flat PDMS surface to NH3 drawn from headspace of 28
NH4OH bottle
Figure 12 shows the results when a flat PDMS sample is used instead of a post
array We clearly observe that the fluorescence response decreases after 60 seconds
which may indicate that the gas movement dislodges the VCP from the surface over
time
Now when we compare the response between the immobilized VCP on a simple
post array and to that of the immobilized VCP on mushroom capped post arrays we
observe empirically that with increasing mushroom cap size which is due to increasing
the 254 nm UV dosage levels to the PMGI layer during fabrication the relative intensity
response increases and response time decreases as observed in Figure 13 Figure 14
and Figure 15
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
18
Figure 13 Fluorescence response of VCP on mushroom capped (200 mJcm2 UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Figure 14 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to NH3 drawn from headspace of 28 NH4OH bottle
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
19
Figure 15 Fluorescence response of VCP on mushroom capped (300 mJcm2 254 nm UV dose) PDMS post array to NH3drawn from headspace of 28 NH4OH bottle
Table 2 shows the comparison of the responses of the different mushroom
capped post array morphologies that are realized due to differing 254 nm UV dosages to
the PMGI layer during the fabrication process
Table 2 Response comparison between simple post array and mushroom capped post arrays to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post 253 3896 70
Immobilized Mushroom cap from 200 mJcm2 UV dose
373 4313 80
Immobilized Mushroom cap from 250 mJcm2 UV dose
451 6896 68
Immobilized Mushroom cap from 300 mJcm2 UV dose
438 9516 35
After initial testing of the responses of the different morphologies of post arrays
we then set about to investigate the response of the different morphologies exposed to
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
20
lowered concentrations of ammonia As viewed in Figure 16 and Figure 17 the intensity
profile and response has changed from the behavior observed previously for higher
concentrations in Figure 13 and Figure 14 The spectral peaks have broadened and the
response speed to ammonia has slowed but still exhibit increases in relative intensities
at full exposure as observed in Table 3
Figure 16 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Figure 17 Fluorescence response of VCP on mushroom capped (250 mJcm2 254 nm UV dose) PDMS post array to 1000 ppm NH3
Also noted in Table 3 is the distinctly different wavelength shifts that are observed but is
only listed for comparison purposes as the spectral shape and intensity profiles are more
important than the wavelength shifts
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
21
Table 3 Response comparison between simple post array and mushroom capped post arrays to 1000 ppm NH3
Sample Peak
wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
Immobilized Simple post -074 10327 180
Immobilized Mushroom cap from 200 mJcm2 UV dose
-371 1258 150
Immobilized Mushroom cap
250 mJcm2 UV dose -203 18945 102
Immobilized Mushroom cap from 300 mJcm2 UV dose
-1166 19444 78
Immobilized Mushroom cap from 350 mJcm2 UV dose
-926 19422 78
Looking at the responses for 5 ppm concentrations the spectral width and shape is
more important in the analysis of the optical response than the peak spectral shift where
there is little difference between the pre-exposure and full-exposure peak wavelengths
as observed in Figure 18 and Figure 19
Figure 18 Fluorescence response of VCP immobilized on simple post array to 5 ppm NH3
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
22
Figure 19 Fluorescence response of VCP on mushroom capped (200 mJcm2 254 nm UV dose) PDMS post array to 5 ppm NH3
The detection results as observed in Table 4 demonstrate similar behavior at 5 ppm to
what is seen at 1000 ppm concentrations with negative spectral shifts As expected the
relative intensity boosts are reduced
Table 4 Response comparison between simple post array and mushroom capped post arrays to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Immobilized Simple post -1169 10570
Immobilized Mushroom cap from 200 mJcm2 UV dose
-279 10369
Immobilized Mushroom cap from 250 mJcm2 UV dose
112 9476
Immobilized Mushroom cap from 300 mJcm2 UV dose
056 9780
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
23
36 Discussion and summary
In summary the main result for this chapter shows that the post array
immobilization technique is robust to flow and enables detection of ammonia at 5 ppm
(which is the lowest concentration currently available for testing)
However we also find that progressing to 254 nm UV dosage levels (beyond 350
mJcm2) results in subsequent fabrication failure of the post arrays The fabrication
failures we observe are likely due to undercutting levels that remove too much
underlying resist to support further processing One possible way to ensure that the
resist layers remain during development after increased irradiation is to increase the
hard bake time and temperature provided to the PMGI layer Another method may be to
change the post spacing and geometries to allow for larger mushroom cap sizes to be
realized from undercutting Another issue encountered is the short time that the VCPs
remain in suspension before precipitating out of the solution Because of this it is difficult
to reproduce the drop casting procedure ensuring that the same quantities of VCP is
deposited Ball milling is proposed as a potential solution to this problem and also to
allow greater penetration of the drop casting solution within the post array However due
to the decrease in mass of VCP crystals the drop cast suspension spreads out into a
larger area and reduces the amount of VCP that remains in the sensing area given by
the spectrometerrsquos focal point resulting in less sensitive sensing surfaces
A final issue identified by this immobilization technique is that given the flexible
nature of the post array the VCPs are ejected from the post array upon physical
manipulation To properly identify the degree of immobilization that is achieved between
the different post array samples a more systematic approach needs to be taken by
measuring the weight difference of the post array after drop cast and physical
manipulation The resulting weight difference would provide the percentage of VCP
immobilization that is achieved for each post array sample
Given that this immobilization technique does not result in complete or long-term
immobilization this method does not appear to be a good way forward in the
immobilization of VCPs
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
24
Chapter 4 Polylactic acid ndash Nanoporous membrane (PLA-NPM)
In this chapter we develop a second physical immobilization method for VCPs
through the creation of polylactic acid based nanoporous membranes (PLA-NPM) to
physically trap the VCPs within the nanoporous membrane (NPM) layers
Polylactic acid (PLA) was chosen as an immobilization material in an attempt to
bring the fabrication process more in line with that of additive manufacturing or 3D
printing PLA is inexpensive and sustainable can maintain physical integrity in power
transformer environments and exhibits little fluorescence in the wavelengths of detection
as observed in Figure 34 and Figure 35 in the Appendix
Similar to the post array method a drop casting solution is used to deposit the
VCPs The procedure is identical with only a change of the solution composition
41 Fabrication of nanoporous membranes (NPMs)
The drop casting solution is prepared by dissolving polylactic acid (PLA) in a
solventnon-solvent co-solution of dichloromethane (DCM) and tetrahydrofuran (THF)
with a volume ratio of 41 The ratio of the solvent (DCM) to non-solvent (THF)
determines the overall porosity of the NPM due to the difference in evaporation rates
between DCM and THF The VCPs are mixed into the solution to form a uniform
suspension Weight ratios of PLA to VCPs of between 12 and 50 are explored The
formula below shows and example preparation to produce a 12 wt PLA-NPM
198119898119892119885119899[119860119906(119862119873))]) + 27119898119892119875119871119860 + 8119898119871119863119862119872 + 21198981198711198791198671198653456789⎯⎯⎯ 22511989811989211987511987111986011988111986211987511990011990312119908119905 119875119871119860 minus 119873119875119872
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast onto a 3D
printed PLA substrate before the VCPs had time to settle out of suspension The
substrate is then suspended approximately 12 cm above a hot plate at a temperature of
100 ordmC to rapidly and uniformly evaporate the solvent co-solution creating NPMs that
immobilize the VCPs
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
25
42 Fabrication results
The drop cast VCP and PLA-NPM is observed with an SEM (FEI Aspex
explorer) and ImageJ software (nihgov) is used to measure the average pore size and
porosity of each sample of PLA-NPM The porosity of the NPM is calculated using
equation
119875119900119903119900119904119894119905119910() = (sum119875119900119903119890 a5b 119860119903119890119886frasl ) lowast 100 (3)
Figure 20 shows the resultant morphology of the VCP PLA-NPMs using both A)
12 wt and B) 48 wt PLA to VCP Since porosity is predominantly determined by the
solvent to non-solvent ratio of the DCM and THF which in our case was set to 41 the
average porosity of all samples was measured to be approximately 50 as shown in
Table 5 From Figure 20 we can observe that the micronano-pores are uniformly
distributed over the entire membrane surface and from Figure 21 we can clearly see that
that VCP content has little impact on the pore formation or distribution
Table 5 Pore count size and area of NPM
Sample of pores Average size of pores (microm)
Area of pores
12 wt PLA-NPM (1) 10333 0474 540
12 wt PLA-NPM (2) 11446 3999 573
48 wt PLA-NPM (3) 7649 0531 501
48 wt PLA-NPM (4) 4533 10851 499
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
26
Figure 20 SEM image A) Porosity resulting from 12 wt PLA B) Porosity resulting from 48 wt PLA (with defect in middle) The white areas are the VCP crystallites immobilized by PLA-NPM (grey)
Figure 21 SEM image of VCP crystals (white) immobilized by PLA-NPM (grey)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
27
43 Experimental methods
Similar to the experimental method for the post arrays Samples of VCP
immobilized by PLA-NPMs on a PLA substrate are inserted inside a 35 mL cork-sealed
quartz cuvette A 30 mW 405 nm deep-violet continuous wave diode laser is used to
excite the material and causes a base emission which peaks at approximately 490 nm
A small spectrometer (PhotonControl SPM-002) records the digital spectrum which is
further computer processed using Matlab Similarly to the first immobilization method
the optical results are analyzed via the data analysis methods developed by Yin et al
[19] A syringe is used to remove the diffused ammonia gas from the headspace of a
28 Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly
concentrated ammonia gas is then pumped into the cuvette at a rate of approximately 1
mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentrations of 50
ppm and 5 ppm Using the calibrated ammonia tanks the gas is pumped into the sample
cuvette at a rate of 194 mLs
44 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected by the PLA-
NPM immobilization technique Figure 22 shows the fluorescence response for a sample
of VCP using 12 wt PLA-NPM while Figure 23 shows the fluorescence response of
VCP using a 48 wt PLA-NPM The NPM immobilization method immobilizes sufficient
amounts of VCPs to cause the sensor cell response to start to saturate as observed in
Figure 23 as compared to the post-based immobilization method To alleviate this issue
the spectrometer exposure rate is reduced but intensity responses cannot be compared
directly due to differences in scaling
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
28
Figure 22 Fluorescence response of immobilized VCP using 12 wt PLA-NPM to NH3 drawn from headspace of 28 NH4OH bottle
Figure 23 Fluorescence response of immobilized VCP using 48 wt PLA-NPM to NH3drawn from headspace of 28 NH4OH bottle
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
29
Table 6 Response comparison between PLA-NPM wt to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost
()
Response time (sec)
(90 of max)
12 wt PLA-NPM (not on substrate) 556 6372 180
12 wt PLA-NPM (on PLA substrate) 245 2477 267
12 wt PLA-NPM (on PLA substrate) 195 2041 279
24 wt PLA-NPM (on PLA substrate) 449 5426 264
48 wt PLA-NPM (on PLA substrate) 624 5123 276
50 wt PLA-NPM (on PLA substrate) 482 5910 240
As shown in Table 6 there is a general increase of response as the percentage of PLA
is increased for samples on a PLA substrate while the largest increase is from a sample
that is not on substrate which is a free floating piece of PLA-NPM with immobilized
VCP The trend of increasing response may be due to the increased amount of PLA
material to retain more the VCP within the NPMs in the sensor area However once the
percentage of PLA exceeds 24 the sensor becomes very difficult to reverse to its
original state as the ammonia molecules may become trapped within the membranes
We again look at the level of ammonia detection for this immobilization technique and
found that it is also able to detect to 5 ppm as shown in Table 7 Again the spectral
width and shape is more important in the analysis of the optical response than the peak
spectral shift at 5 ppm ammonia concentrations where there is little difference between
the pre-exposure and full-exposure peak wavelengths as observed in Figure 24 and
Figure 25
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
30
Table 7 Response comparison between PLA-NPM wt to 5 ppm NH3
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (sec)
(90 of max)
12 wt PLA-NPM (on PLA substrate) 037 870 270
12 wt PLA-NPM - P1 (on PLA substrate) -389 10536 NA
24 wt PLA-NPM (on PLA substrate) 148 956 NA
50 wt PLA-NPM (on PLA substrate) 482 1047 60
Figure 24 Fluorescence response of immobilized VCP using 24 wt PLA-NPM to 5 ppm NH3
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
31
Figure 25 Fluorescence response of immobilized VCP using 50 wt PLA-NPM to 5 ppm NH3
45 Discussion and summary
As with the post arrays the PLA-NPM immobilization technique is dependent on
the amount of VCPs that are immobilized within the narrow focal point of the
spectrometer sensing area It is also discovered through experimentation that the
experimental setup has a degree of manipulation to it to allow for varying degrees of
response for any sample This is a major drawback discovered with this experimental
setup Since the quality of the response highly dependent upon the amount of sample
that is able to be present in focal pathway of the spectrometer and the degree of focus
that can be achieved Every effort is made to fix the optical setup so that every sample is
measured with the same conditions and without altering the optical setup between
samples However it is discovered that the optical setup may be optimized for each
sample
In terms of use as a sensor it is found that 12 wt to 88 wt is the weight ratio
of PLA to VCP to provide ammonia detection of 5 ppm long-term immobilization and
greatest degree of reversibility allowing sensors employing this immobilization technique
to be repeatedly reused
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
32
Chapter 5 3D printed ammonia sensor
In this chapter we look at the first fully fluidic prototype ammonia sensor
application that is created for the detection of ammonia using PLA-NPMs and cyclic
olefin copolymer based nanofibers (hereby known as COC-NFs) to immobilize the
VCPs We discuss the fabrication of the prototypes via 3D printing of the sensor cell and
their characterization along with the optical test method and results
51 Fabrication
In addition to the technique presented in Chapter 4 PLA is also commonly
employed in 3D printing [26] However COC is chosen instead as the 3D printing
material for the fluidic sensor cells presented in this chapter for several reasons Firstly
while transparent PLA stock is available it is found that after printing the transparency of
PLA turns fairly opaque to light transmission in the desired wavelengths and requires the
creation of a fluidic cell that is comprised of both PLA and a glass transmission window
for optical detection However printed COC maintains near perfect optical transmission
in the required wavelength region and does not absorb or fluoresce in that region as
observed in Figure 36 and Figure 37 in the Appendix Secondly COC can maintain its
integrity without deformation in higher temperatures than PLA and can be printed as one
sealed device
Prototype designs of the fluidic cell are created in Solidworks and Autocad and
then imported to the 3D COC printer software Fluid Factory (Dolomite Fluid Factory)
which creates the layers to be printed Figure 26 illustrates the CAD drawing
representations of the top views of the top layer on the left and the bottom layer with a
microfluidic layer The size of the prototype fluidic sensor is chosen to match the size and
allowable geometries that are present with the optical setup and therefore dictated the
overall size of the cell The fluidic layer depth is set to the minimum depth possible by
the 3D printerrsquos capabilities Therefore the prototypes use a microfluidic layer that is 300 microm
in depth with the entire cell measuring 18x7x60 mm (WxHxL) The majority of the height
is attributed to the inlet and outlet ports This is because a sufficient port length is
required for the attachment of tubing that is able to resist backflow and attach with
minimal amounts of adhesive and while maintaining its physical attachment strength
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
33
Figure 26 Top (left) and bottom (right) views of 3D printed sensor cell
The drop casting solutions for the PLA-NPMs are prepared exactly according to
the procedures outlined in Chapter 4 The drop casting solution is prepared by dissolving
polylactic acid (PLA) in a solventnon-solvent co-solution of dichloromethane (DCM) and
tetrahydrofuran (THF) with a volume ratio of 41 The VCPs are mixed into the solution
to form a uniform suspension
As a method of more closely integrating the VCP solution with the base COC
substrate new solutions are investigated While there has been research into forming
porous COC membranes [22 23] these methods of creating membranes are not
compatible with this method of immobilization We instead follow a similar technique as
used for the creation of PLA-NPMs through a combination of solvents and non-solvents
to dissolve the COC into solution Through experimentation a suitable solventnon-
solvent combination is found in the form of cyclohexane and benzaldehyde in a ratio of
61 by volume While many other less non-polar non-solvents are experimented with to
act as the non-solvent only benzaldehyde is able to be mixed with the cyclohexane and
COC without causing the immediate re-solidification of the COC out of the solution The
VCPs are mixed into the solution to form a uniform suspension
Once the solutions are thoroughly mixed and the VCPs are in uniform
suspension the solutions are drawn into a syringe and quickly drop cast into the fluidic
channel of a 3D printed COC substrate before the VCPs had time to settle out of
suspension The substrate is then suspended approximately 12 cm above a hot plate at
a temperature of 100 ordmC to rapidly and uniformly evaporate the solvent co-solution
creating NPMs that immobilize the VCPs
Two methods are employed to create the 3D printed COC fluidic cells The first
method involves printing the bottom fluidic layer and top inletoutlet layers separately
and the PLA-VCP or the COC-VCP solution is drop cast into the fluidic layer After the
evaporation of the solvent co-solution the two layers are bonded together employing the
technique discussed by Keller et al [20] where a mixture of cyclohexane and acetone is
used to make the bonding sides of each layer tacky enough to bond them together The
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
34
second method is to print the bottom fluidic layer and then pause the printing The PLA-
VCP or COC-VCP solution is drop cast into the fluidic layer and then after the
evaporation of the solvent and non-solvents the top layer is immediately printed overtop
creating a completely sealed fluidic chamber
52 Fabrication results
While initially it is assumed that the PLA-VCP drop cast solution would form the
intended PLA-NPMs as observed in Figure 20 and Figure 21 it turned out that instead
the PLA acted more as a glue to adhere the VCPs to the surface of the COC fluidic cell
instead and did not form the PLA-NPM as observed in Figure 27 The most noticeable
visual difference is that the VCPs are no longer trapped beneath gas porous NPMs but
stuck on and in between PLA This change suggests a reduction of gas access to the
VCP crystal surfaces
At the time of this writing it is unclear the reason behind the failure to form the
intended PLA-NPM but could be due to any number of unintended chemical interactions
between the aqueous suspension and the COC surface or the failure of having a PLA
substrate to help form the proper bonds to facilitate the formation of the NPM during the
solventnon-solvent evaporation
Figure 27 SEM image of PLA-VCP mixture in COC fluidic channels Left α-Zn[Au(CN)2]2 Right β- Zn[Au(CN)2]2 which no longer exhibits the intended formation of NPM to immobilize the VCPs
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
35
It is further discovered that when attempting to drop cast using solutions that
contain the α- Zn[Au(CN)2]2 polymorph with hexagonal crystals two unintended
situations may occur When drop cast the resulting distribution of the VCPs is denser
and more uniform However what negated any positive effects is that the PLA often
overly interferes or envelops the crystals and thereby reduces the available binding sites
for ammonia This results in poor or non-reactive sensors as observed from Figure 28
Figure 28 SEM image of α-Zn[Au(CN)2]2 PLA-VCP Left PLA covering over VCPs Right PLA enveloping VCP crystals
When the solution of α- Zn[Au(CN)2]2 polymorph and COC is drop cast we
surprisingly find that it the VCP is not immobilized by an NPM but instead by nanofibers
(NF) as observed in Figure 29 The NFs ranged in size up to 500 nm in width and of
varying lengths bonding crystals together large pieces of COC and the COC substrate
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
36
Figure 29 SEM images of α-Zn[Au(CN)2]2 VCP immobilized by COC nanofibers (thin filaments linking hexagonal VCP crystals)
53 Experimental methods
Similar to the experimental method for the post arrays and PLA-NPMs the
samples of Zn[Au(CN)2]2 VCP are immobilized by COC-NFs and the PLA-NPMs in the
fluidic channel The 3D printed COC cell is used as the replacement to the cuvette A 30
mW 405 nm deep-violet continuous wave diode laser is used to excite the material and
causes a base emission which peaks at approximately 480 nm A small spectrometer
(PhotonControl SPM-002) records the digital spectrum which is further computer
processed using Matlab Similarly to the other immobilization methods the optical
results are analyzed via the data analysis methods developed by Yin et al [19] A
syringe is used to remove the diffused ammonia gas from the headspace of a 28
Ammonium Hydroxide (NH4OH) solution bottle Next 10 mL of this highly concentrated
ammonia gas is then pumped into the cuvette at a rate of approximately 1 mLsec
The experiment is repeated using calibrated gas tanks of ammonia mixed with N2
as the balancing gas for the concentration of 1000 ppm Whereas calibrated gas tanks of
ammonia mixed with lab air as the balancing gas is used to test at concentration of 5
ppm Using the calibrated ammonia tanks the gas is pumped into the sample cuvette at
a rate of 194 mLs
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
37
A second experimental setup is made for testing of ammonia dissolved in silicone
oil The setup used is the same as the previous experimental setup however with the
change that the oil is drawn out of an oil reserve using a micro fluidic pump at a rate of
10 mLmin into the fluidic cell Once the cell is filled the oil is held there for the duration
of the experiment
54 Optical results
Optical testing to the exposure of headspace ammonia (NH3) shows that the
optical and fluorescence characteristics of the VCP is largely unaffected immobilization
in our sensor design prototypes However one obvious change in response is the large
increase of response time as observed in Figure 30 and Figure 31 Previous
immobilizations had VCP response times in the seconds to minutes whereas the VCP
responses in the fluidic cells take upwards of an hour or longer to achieve the same
levels of exposure
Figure 30 Fluorescence response of immobilized VCP (PLA-NPM) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
38
Figure 31 Fluorescence response of immobilized VCP (COC-NF) in COC fluidic cell to NH3 drawn from headspace of 28 NH4OH bottle Response is due to diffusion of NH3 through the fluidic cell
Table 8 Response comparison between COC fluidic cells to NH3 drawn from headspace of 28 NH4OH bottle
Sample Peak wavelength shift (nm)
Relative intensity boost ()
Response time (90 of max)
COC PLA-NPM β polymorph 217 5983 40 minutes
COC-NF α polymorph 199 2278 258 minutes
Finally we look at the results that we achieve from exposing the fluidic cell to
ammonia saturated silicone oil The results presented are from the technique that was
developed by Yin et al [19] and can be observed in Figure 32 This second technique is
required for the detection of low concentrations of ammonia and what is used for the
detection for not only the oil-based experiments but also throughout this thesis for the
detection of the 5 ppm gas concentrations The change of detection method is required
as at these low gas concentrations as the spectral shifts and relative intensities are too
small to be determined visually From Figure 32 we observe that once the oil is drawn
into the sensing chamber the response rises quickly and comes to a steady state within
a few minutes
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
39
Figure 32 Response of samples exposed to silicone oil which ammonia was bubbled through for 1 hour Left 12 wt PLA-NPM Right COC-NF
55 Discussion and summary
The resulting microfluidic sensor cell and processes outlined in this chapter show the
successful immobilization of the VCP as well as detection of ammonia in both gas
phase and dissolved into a fluid Examination of VCP morphology reveals its role in the
effectiveness of different immobilization techniques
Using the immobilization technique employing PLA-NPMs results in most sample
cells being less responsive to similar levels of ammonia exposure as to PLA-NPMs on
PLA substrates There is also a noticeable drop in sensitivity for the COC-NFs from the
PLA-NPMs in our prototype sensor cells From our discoveries on how the PLA-VCP
suspension behaved when drop cast into the COC fluidic cell we see that this result
should not be unexpected and points to the important characteristics of the physical
morphology that comes into play for immobilization in COC fluidic cells
When we look at the SEM images of the resulting immobilization of both the a
and b polymorphs using the PLA-VCP solution we see marked differences as observed
in Figure 27 This may help to explain why when we use the b polymorph we have a
reduction in sensitivity as the crystals are now clumped together and no longer held
within NPMs Figure 28 shows how when using the a polymorph the PLA seems to
prefer to envelope the VCP crystals causing the resulting sensor to be non-sensing
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
40
Therefore using PLA-VCP drop cast solution with the a polymorph in a COC based cell
is determined to be not an effective or useful immobilization technique
When we look at the immobilization of the VCP when using a COC based
suspension using the a polymorph we find resulting immobilization to involve the
nanofibers as observed in Figure 29 We did not have a chance to observe the resulting
immobilization from the b polymorph as we did not have access to the b polymorph at
the time to compare
It is observed that the size or width of the fluidic channel resulted in the printer
creating the fluidic layer as more of a mixer than a straight flowing channel when printing
the entire chip in a single print job as observed in Figure 33 While this is avoided when
printing the top and bottom layers separately the binding of the layers proved
challenging to maintain a fluid tight seal and without clogging the fluidic layer
Figure 33 COC fluidic cell with immobilized VCP fluorescing under 405 nm laser light
It is shown that these fluidic cells are able to detect ammonia that has been
dissolved in silicone oil similar to that what is found inside power transformers Being
able to detect ammonia in the liquid phase extends the capabilities of this type of
ammonia sensor and shows that the presented immobilization technique can unlike
many other sensors based on previously existing techniques measure ammonia in liquid
phase (eg oil)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
41
Chapter 6 Conclusions and Future work
Table 9 Comparison of immobilization techniques N2 used as balance gas instead of air
Technique Customization Concentration
50000 ppm
1000 ppm 50 ppm 5 ppm
Post array Simple Clear positive
response
Weak positive
responseinconclusive
No data Weak positive
responseinconclusive response Mushroom
200 mJcm2 Clear
positive response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
responseinconclusive
Mushroom 250 mJcm2
Clear positive
response
Clear positive
response
Weak positive
responseinconclusive
Weak positive
response
Mushroom 300 mJcm2
Clear positive
response
Clear positive
response
No data Weak positive
response PLA-NPM 12 wt
(88 VCP) Clear
positive response
Clear positive
response
Clear positive
response
Weak positive
response
12 wt ndash P1 (88 VCP)
Clear positive
response
Clear positive
response
Clear positive
response
Weak positive
response 24 wt
(76 VCP) Clear
positive response
Clear positive
response
No data Weak positive
responseinconclusive
48 wt (52 VCP)
Clear positive
response
Clear positive
response
No data No data
50 wt (50 VCP)
Clear positive
response
Clear positive
response
No data Weak positive
responseinconclusive
COC-NF COC PLA-NPM β polymorph
Clear positive
response
Clear positive
response
No data Negative response
COC-NF α polymorph
Clear positive
response
Clear positive
response
No data Negative response
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
42
Table 9 shows a summary of the different immobilization techniques that are
presented in this thesis showing the levels of response in the detection of ammonia at
given concentrations in air The exception is for the results for 1000 ppm in which the
balancing gas used during testing was N2 instead of air
We see from Table 9 that both the higher 254 nm UV dose post arrays and the
higher VCP percentage PLA-NPM immobilization techniques result in a sensing surface
that is able detect relatively low concentration levels of 5 ppm However the simple post
arrays low VCP percentage PLA-NPM and COC cell result in a sensing surface that
has experimentally been shown to only detect ammonia concentration levels of 1000
ppm The determination of the results for the lower concentration levels below 1000
ppm are complied through the comparison of data obtained through both methods of
data analysis While some samples may show weak positive responses to lower
concentrations from one data analysis method there either is insufficient data points or
conflicts between the two methods to prove the results to be conclusive
While it was sought to experiment equally with both the a and b polymorphs of
the VCP the b polymorph was the only polymorph that was used throughout all
immobilization techniques It is only the COC cells in which both the a and b polymorphs
are used It is also for these cells where it is discovered that the polymorph morphology
became an important consideration With the creation of these fluidic cells we have also
been able to show that the sensor cells are able to detect ammonia that is dissolved in
silicone oil which is promising for use of the sensor in detecting ammonia in both gas
and liquid samples
It is of great consideration to pick immobilization materials that do not absorb
reflect or fluoresce at the wavelengths of issue However it is determined that all
immobilization materials did in fact slightly interfere with the resulting spectral response
For example the un-immobilized base material has an emission peak at 480 nm
However once immobilized the base emission peak shift up to approximately 490 nm for
the post arrays and the PLA-NPMs While it is not the focus of this thesis to look at the
optical detection scheme and data analysis algorithms through experimentation it is
found that the data analysis algorithm can be tuned or manipulated to change the type of
response that is found With every immobilization method the unexposed and exposed
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
43
spectral peaks shifted wavelengths from what is observed in the un-immobilized
samples
In conclusion in this thesis we show development of several immobilization
techniques for VCPs aimed at improving the sensitivity reducing the cost of fabrication
and allowing the sensors surface to be able to detect ammonia in fluid flow We have
shown that through the micromachining of PDMS we are able to create post arrays with
mushroom capped tops that are able to effectively immobilize VCPs within the post array
as well as detect ammonia at low concentrations of 5 ppm which is close to the required
lower detection limit of 1 ppm The major drawback to the post-based immobilization
method is that through physical manipulation of the post array sensing surface VCPs
are lost thereby reducing the sensing surfacersquos sensitivity over time This also highlights
that the post-based immobilization technique can only be used for sensing ammonia as
a gas as any liquid may slowly remove the VCPs from the surface We have shown that
we are able to immobilize VCPs within PLA-NPMs resulting in a sensor surface that
provides for the long-term immobilization of the VCPs Using this technique surfaces are
also able to detect ammonia that has been dissolved in fluids and that can detect
ammonia at low concentrations of 5ppm which is close to the required detection limit of
1 ppm In addition we have shown through the combination of solutions consisting of
PLA-VCP and COC-VCP we are able to immobilize VCPs into the 3D printed fluidic
COC cell that can be used in the detection of ammonia as both a gas and dissolved in
fluid
While all immobilization techniques show degrees of promise we conclude that
the most promising of all the techniques is the PLA-NPM immobilization technique The
PLA-NPM immobilization technique demonstrates long-term immobilization the ability to
directly detect ammonia dissolved in oil and the ability to detect low levels of ammonia
in the concentration amount of 5 ppm This immobilization technique should be the focus
of all future work for the immobilization of VCPs for use in gas sensors
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
44
61 Future work
The work presented in this thesis show the development of several novel
methods for the immobilization of VCPs However some key issues need to be
addressed by future work
611 Post Arrays
bull Investigate different methods of surface activation to promote increased
VCP bonding to the surface
bull Investigate new solvents to form better VCP suspensions
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Test the effectiveness of immobilization technique with the a polymorph
of VCP
bull Develop metric (ie weight difference) to determine degree of
immobilization of VCPs for different post arrays based on the amount of
VCPs that are ejected from post arrays after drop casting
612 PLA-NPMs and 3D printed fluidic cells
bull Improve process methodologies to realize a greater control and
reproducibility of the amount of VCPs deposited and into a controlled and
confined sensor area
bull Improve optical setup so that no manipulation is required between
samples and standardizing 3D printing process so that sensor area is
defined in correlation to optical detection area on chip
bull Modify fluidic layer to improve flow conditions around or over sensing
VCP-NPMsNFs
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
45
bull Continue investigation of VCP physical morphology and its role in
immobilization and formation of NPMs and NFs
bull Test the effectiveness of immobilization on PLA substrate using PLA-
NPMs with the a polymorph of VCP
bull Further test the effectiveness of immobilization for COC cells using the b
polymorph of VCP
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
46
References
[1] E Dornenburg W Strittma Monitoring oil-cooled transformers by gas-analysis Brown Boveri Rev 1974 Vol 61 No 5 pp 238-247
[2] M Duval A Review of faults detectable by gas-in-oil analysis in transformers IEEE Elect Insul Mag 2002 Vol 18 No 3 pp 8-17
[3] K Zakrzewska ldquoMixed oxides as gas sensorsrdquo Thin Solid Films 2001 Vol 391 Issue 2 pp 229-338
[4] R Binions A J T Naik ldquoMetal oxide semiconductor gas sensors in environmental monitoringrdquo Semiconductor Gas Sensors Woodhead Publishing Series in Electronic and Optical Materials 2013 pp 433-466 httpsdoiorg10153397808570986654433
[5] C Wang X Li F Xia H Zhang J Xiao ldquoEffect of V2O5-content on electrode catalytic layer morphology and mixed potential ammonia sensor performancerdquo Sensors and Actuators B Chemical 2016 Vol 223 pp 653-668 httpsdoiorg101016jsnb201509145
[6] A Marikutsa A Sukhanova M Rumyantseva A Gaskov ldquoAcidic and catalytic co-functionalization for tuning the sensitivity of sulfated tin oxide modified by ruthenium oxide to ammonia gasrdquo Sensors and Actuators B Chemical 2018 Vol 255 Part 3 pp 3523-3532 httpsdoiorg101016jsnb201709186
[7] L Huixia L Yong L Lanlan T Yanni Z Qing L Kun ldquoDevelopment of ammonia sensors by using conductive polymerhydroxyapatite composite materialsrdquo Materials Science and Engineering C 2016 Vol 59 pp 438-444 httpsdoiorg101016jmsec201510036
[8] S Sharma S Hussain S Singh SS Islam ldquoMWCNT-conducting polymer composite based ammonia gas sensors A new approach for complete recovery processrdquo Sensors and Actuators B Chemical 2015 Vol 194 pp 213-219 httpsdoiorg101016jsnb201312050
[9] L Kumar I Rawal A Kaur S Annapoorni ldquoFlexible room temperature ammonia sensor based on polyanilinerdquo Sensor and Actuators B Chemical 2017 Vol 240 pp 408-416 httpsdoiorg101016jsnb201608173
[10] Y Cheng Q Feng M Yin C Weng Y Zhou ldquoA fluorescence and colorimetric ammonia sensor based on a Cu(II)-27-bis(1-imidazole)fluorene metal-organic gelrdquo Tetrahedron Letters 2016 Vol 57 Issue 34 pp 3814-3818 httpsdoiorg101016jtetlet201607013
[11] F Tavoli N Alizadeh ldquoOptical ammonia gas sensor based on nanostructure dye-doped polypyrrolerdquo Sensors and Actuators B Chemical 2013 Vol 176 pp 761-767 httpsdoiorg101016jsnb201209013
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
47
[12] M J Katz T Ramnial H Yu D B Leznoff ldquoPolymorphism of Zn[Au(CN)2]2 and Its Luminescent Sensory Response to NH3 Vaporrdquo JACS articles 2008
[13] B F Hoskins R Robson N V Y Scarlett ldquoSix Interpenetrating Quartz-Like Nets in the Structure of ZnAu2(CN)4rdquo Angewandte Chemie International Edition in English 1995 Vol 34(11) pp 1203-1204
[14] J S Ovens D B Leznoff ldquoThermally triggered elimination of bromine from Au(III) as a path to Au(I)-based coordination polymersrdquo Dalton Transactions 2011 40 4140
[15] D Sameoto and C Menon ldquoA low-cost high-yield fabrication method for producing optimized biomimetic dry adhesivesrdquo Journal of Micromechanics and Microengineering 19 (2009) 115002 (7pp) stacksioporgJMM19115002
[16] J Kahn C Menon ldquoDry adhesives with sensing featuresrdquo Smart materials and Structures IOP Publishing 2013 Vol22(8) p085010
[17] M Hu W Kang Z Li S Jie Y Zhao L Li et al ldquoZinc(II)phophyrin-poly(lactic acid) nanoporous fiber membrane for ammonia gas detectionrdquo J Porous Mater (2016) 23911-917 DOI 101007s10934-016-0148-5
[18] D Stevens B Gray D Yin G Chapman D B Leznoff ldquoPost arrays for the immobilization of vapochromic coordination polymers for chemical sensorsrdquo In Proc 2017 IEEE SENSORS 2017 pp 1-3 httpsdoiorg101109ICSENS20178234080
[19] D Yin G Chapman D Stevens B Gray D B Leznoff ldquoDetection of low concentration ammonia using differential laser induced fluorescence on vapochromic coordination polymersrdquo In Proc SPIE West on Photonic Instrumentation Engineeringrsquo01 2018 105390K
[20] N Keller T M Nargang M Runck F Kotz A Striegel K Sachsenheimer D Klemm K Laumlnge M Worgull C Richter D Helmer B E Rapp ldquoTacky cyclic olefin copolymer a biocompatible bonding technique for the fabrication of microfluidic channels in COCrdquo Lab Chip 2016 16 1561 DOI 101039c5lc01498k
[21] Z Qi H Yu Y Chen M Zhu ldquoHighly porous fibers prepared by electrospinning a ternary system of nonsolventsolventpoly(L-lactic acid)rdquo Materials Letters 2009 Vol 63 Issue 3-4 415-418 httpsdoiorg101016jmatlet200810059
[22] Y Li C T Lim M Kotaki ldquoStudy on structural and mechanical properties of porous PLA nanofibers electrospun by channel based electrospinning systemrdquo Polymer 2015 Vol 56 572-580 httpsdoiorg101016jpolymer201410073
[23] B Timmer W Olthius A Berg ldquoAmmonia sensors and their applicationsmdasha reviewrdquo Sensors and Actuators B Chemical 2005 Vol 107 Issue 2 pp 666-677 httpsdoiorg101016jsnb200411054
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
48
[24] M Gel S Kandasamy K Cartledge D Haylock ldquoFabrication of free standing microporous COC membranes optimized for in vitro barrier tissue modelsrdquo Sensors and Actuators A Physical 2014 Vol 215 pp 51-55 httpsdoiorg101016jsna201310018
[25] M Dogu N Ercan ldquoHigh performance cyclic olefin copolymer (COC) membranes prepared with melt processing method and using of surface modified graphitic nano-sheets for H2CH4 and H2CO2 separationrdquo Chemical Engineering Research and Design 2016 Vol 109 pp 455-463
[26] VE Kuznetsov AN Solonin OD Urzhumtsev R Schilling AG Tavitov rdquoStrength of PLA Components Fabricated with Fused Deposition Technology Using a Desktop 3D Printer as a Function of Geometrical Parameters of the Process ldquo Polymers 2018 10 313
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
49
Appendix
Fluorescence spectrum data
Figure 34 Emission spectra of PLA between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 35 Fluorescence spectra of PLA between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
50
Figure 36 Emission spectra of COC between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 37 Fluorescence spectra of COC between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)
51
Figure 38 Emission spectra of PDMS between 200 and 600 nm illuminated with UV-Vis-NIR light source using 275-375 nm band pass color filter Captured from spectrometer (Flame Ocean Optics)
Figure 39 Fluorescence spectra of PDMS between 400 and 600 nm Captured from spectrometer (Flame Ocean Optics)