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RHEOLOGICAL MEASUREMENTS
BY AFM OF THE FORMATION
OF POLYMER NANOFIBERS
M. M. Yazdanpanah, M. Hosseini, S. Pabba, S. M. Berry, V. V. Dobrokhotov,
A. Safir, R. S. Keynton and R. W. Cohn
ElectroOptics Research Institute & Nanotechnology Center
University of Louisville
The Processing Parameter P: Key material parameter that predicts nanofiber dimensions
Measurements of material constants that comprise P:Surface tension, evaporation rate, viscosity
Using constant diameter nanoneedles for measuring P and drawing of nanofibers
RHEOLOGICAL MEASUREMENTS BY AFM OF THE FORMATION OF POLYMER NANOFIBERS
PROCESSING PARAMETER AND FIBER FORMATION
Fiber diameter depends on
as well as droplet diameter
(Tripathi and McKinley)
P
P = 0.01
P
P = 0.05
Rm
id/R
0R
mid
/R0
P
P = 0.01
P
P = 0.05
P
P = 0.01
P = 0.05
Rm
id/R
0
= 0 P = 0.005P
P = 0.01
P
P = 0.05
Rm
id/R
0
P
P = 0.01
P
P = 0.05
P
P = 0.01
P
P = 0.05
Rm
id/R
0R
mid
/R0
P
P = 0.01
P
P = 0.05
P
P = 0.01
P = 0.05
Rm
id/R
0
= 0 P = 0.005
Evaporation rate x viscosityP =
Surface tension
Harfenist et al. Nanoletter 2004
CONSTANT DIAMETER NANONEEDLE AFM TIPS FOR PULLING POLYMERIC NANOFIBER
Thinnest fibers are drawn with thinnest tips
Needles on AFM tips point to interactive measurementof processing parameter while drawing fibers
5 m
100 nm
Needle
Polymerfiber
Yazdanpanah et. al., JAP 2005
AFM MEASUREMENT OF
Surface tension
Evaporation rate
ViscosityTo get processing parameter
using constant diameter nanoneedles
Circumference needed to extract surface tension
On tapered tips, wetting force grows unstably with depth
Viscous drag force is directly related to insertion depth
ADVANTAGES OF CONSTANT DIAMETER NEEDLES FOR AFM ANALYSIS OF LIQUIDS
cos2 rFe
10m
SELECTIVE GROWTH OF LONG NEEDLES
Time lapse images show growth of a 70 micron long needle
Fs
Fe < FS
Fe = FS
Fe = FS cos(
Fs
Fe < FS
Fs
F < FS
Fr = FS
Fe = FS cos(
Fs
Fe < FS
Fs
Fe < FS
Fe = FS
Fe = FS cos(
Fs
Fe < FS
Fs
F < FS
Fr = FS
Fe = FS cos(
MEASUREMENT OF SURFACE TENSION
PLUS CONTACT ANGLE
Surface tension is found from
Contact angle is found from
cosre FF
SEM images of needle being retracted from vacuum oil
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
Water
Chlorobenzene
Vacuum Oil
Dibasic ester
Distance (µm)
-50
0
2 1 0
-50
0
-50
0
-50
0
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
Water
Chlorobenzene
Vacuum Oil
Dibasic ester
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
Water
Chlorobenzene
Vacuum Oil
Dibasic ester
Distance (µm)
-50
0
2 1 0
-50
0
-50
0
-50
0
-50
0
2 1 0
-50
0
-50
0
-50
0
FrFe
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
Water
Chlorobenzene
Vacuum Oil
Dibasic ester
Distance (µm)
-50
0
2 1 0
-50
0
-50
0
-50
0
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
Water
Chlorobenzene
Vacuum Oil
Dibasic ester
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
Water
Chlorobenzene
Vacuum Oil
Dibasic ester
Distance (µm)
-50
0
2 1 0
-50
0
-50
0
-50
0
-50
0
2 1 0
-50
0
-50
0
-50
0
rFF Sr 2
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
Water
Chlorobenzene
Vacuum Oil
Dibasic ester
Distance (µm)
-50
0
2 1 0
-50
0
-50
0
-50
0
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
Water
Chlorobenzene
Vacuum Oil
Dibasic ester
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
-50
0
4 3 2 1 0
Distance (µm)
-50
0
-50
0
-50
0
F/
D(m
N/m
)
Water
Chlorobenzene
Vacuum Oil
Dibasic ester
Distance (µm)
-50
0
2 1 0
-50
0
-50
0
-50
0
-50
0
2 1 0
-50
0
-50
0
-50
0
TYPICAL F-D CURVES FOR MEASURING SURFACE TENSION AND CONTACT ANGLE
5 m
100 nm
5 m
300nm
Ag2Ga alloy, dual-diameter
needle
Parylene coated, single-diameter
needle
Vertical axis scaled by circumference to be in units of surface tension
Surface tension (mN/m)
Surface tension
published (mN/m)
Contact angle(degrees)
Bare Coated Bare Coated
Water 74.6 74.2 72.8 51 ± 2 62 ± 2
Chlorobenzene 33.1 35.4 33.0 27± 3 21 ± 3
Dibasic ester 37.5 37.4 35.6 24 ±1 22 ± 1
Vacuum oil 36.8 36.9 35 22 ± 1 27 ± 1
Isopropanol 24.9 24.8 23 20 ±3 19 ± 3
Toluene - 30.3 27.9 - 32 ± 2
SURFACE TENSION AND
CONTACT ANGLE
Measured and published values of surface tension in agreement
Contact angles differ by up to 11o for bare and coated needles
Each measurement is the average of at least 20 measurements. The deviation reported is peak-to-peak.
MEASURING EVAPORATION RATE
AFM is sensitive to sub-nanometer changes in surface height between repetitive scans
AFM data is in good agreement with TGA data
-20
0
nN
2 1 0µm
l
AFM(m/s)
TGA (m/s)
Acetone 1.45 ± 0.05 1.02
IPA 0.32 ± 0.01 0.178
CLB 0.11 ± 0.01 0.098
DI 0.027 ± 0.001 0.036
DMF 0.0115 ± 0.0005 0.0094
DBE 0.00026 ± 0.0001 0.00022
Vacuum oil ~ 0 ~0
VISCOUS DRAG FORCE ON NEEDLELOWERS Q OF THE VIBRATING CANTILEVER
Measurements of Q-damping vs. needle insertion depth are fit to a model of drag force to give one value of viscosity
Measurements of glycerol-water track literature and our own shear plate viscometer measurements over three orders of magnitude
Needle is rugged: Same needle used for every measurement!!
0 20 40 60 80 100
1
10
100
1000
Vis
cosi
ty (
cP)
Concentration (wt.%)
20o C
30o C
AFM data at 22 oC
Viscometer data 24 oC
0.0 5.0x10-6 1.0x10-5 1.5x10-5
0.0
0.5
1.0
1/Q
Distance (m)
(a) (b)
0 20 40 60 80 100
1
10
100
1000
Vis
cosi
ty (
cP)
Concentration (wt.%)
20o C
30o C
AFM data at 22 oC
Viscometer data 24 oC
0.0 5.0x10-6 1.0x10-5 1.5x10-5
0.0
0.5
1.0
1/Q
Distance (m)
(a) (b)
99.5 wt %
80 wt %
13.4 wt %
0 20 40 60 80 100
1
10
100
1000
Vis
cosi
ty (
cP)
Concentration (wt.%)
20o C
30o C
AFM data at 22 oC
Viscometer data 24 oC
0.0 5.0x10-6 1.0x10-5 1.5x10-5
0.0
0.5
1.0
1/Q
Distance (m)
(a) (b)
0 20 40 60 80 100
1
10
100
1000
Vis
cosi
ty (
cP)
Concentration (wt.%)
20o C
30o C
AFM data at 22 oC
Viscometer data 24 oC
0.0 5.0x10-6 1.0x10-5 1.5x10-5
0.0
0.5
1.0
1/Q
Distance (m)
(a) (b)
Glycerolin water
Fiber length increase over an order of magnitude closely following a log-log trend
Liquid with these low value of P does not form stable fibers or strings, but were used to enable cleaner, more ideal first-time measurements
These results point towards the controlled, interactivedrawing of nanofibers with these needles and higher P liquids
STRONG CORRELATION BETWEEN FIBER LENGTH AND PROCESSING PARAMETER
(a) (b)
10-10 10-8 10-6 1x10-4
102
103
lb
tb
t b (s)
l b (n
m)
P
1 10
0.1
1
Concentration (wt.%)
0 2 4 6 8
-160
-80
0
nN
1.51.00.50.0
Sec
time (S)
Time (s)
Fo
rce
(n
N)
tb
(a) (b)
10-10 10-8 10-6 1x10-4
102
103
lb
tb
t b (s)
l b (n
m)
P
1 10
0.1
1
Concentration (wt.%)
0 2 4 6 8
10-10 10-8 10-6 1x10-4
102
103
lb
tb
t b (s)
l b (n
m)
P
1 10
0.1
1
Concentration (wt.%)
0 2 4 6 8
-160
-80
0
nN
1.51.00.50.0
Sec
time (S)
Time (s)
Fo
rce
(n
N)
tb-160
-80
0
nN
1.51.00.50.0
Sec
time (S)
Time (s)
Fo
rce
(n
N)
tb
P
AFM F-T curves of breakup length
Processing Parameter PLength (m)
lb
Constant diameter nanoneedles were used to measure the Processing Parameter P as well as to show the correlation between P and fiber length
For simple liquids, surface tension, evaporation rate and viscosity were measured with reasonable to high accuracy
For random chain polymeric liquids viscosity was very low, but this may accurately reflect viscosity for the nanoscale
displacements of the thermally-actuated AFM cantilevers
The needles are very rugged and reliable for liquid studies—Only 4 needles were used for the entire study!
SUMMARY
RHEOLOGICAL MEASUREMENTS BY AFM