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7/31/2019 Characterization & Identification of Polymers Presentation
1/42
1To ic IV.1 & 2 Courtesy of University of Leoben, Austria
Topic IV:Structural Characterization and Identification of Polymers
IV.1. Thermoanalytic methods- Differential thermal analysis (DTA) & differential scanning calorimetry (DSC)- Thermogravimetric analysis (TGA)- Thermomechanical analysis (TMA)
IV.2. Spectroscopic methods- IR Spectroscopy
IV.3. Microscopic methods- Optical/light Microscopy- Scanning Electron Microscopy
IV.4. Diffraction methods- X-Ray Diffraction
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Differential Thermal Analysis (DTA) & Differential Scanning Calorimetry (DSC)Methods based on measurement of heat consumed (endo) up or released (exo)to the surrounding per unit time during isothermal (hold), heating or cooling
processes.
Thermogravimetric Analysis (TGA)Measurement of changes of polymer weight as a function of temperature.
Thermomechanical Analysis (TMA)Measurement of dimensional changes during heating or cooling
Thermoanalytic Methods
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Thermoanalytic Methods - DTA
Differential Thermal Analysis (DTA)
Sample (~10mg) pan and reference pan are placed in an oven. The oven is usually heated or cooled at a rate ranging from 0.1 to 100 K/min.
Temperature difference (T) between sample and reference pan measured and recorded.
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Thermoanalytic Methods DTA/DSC
380 400 420 440 460-15
-10
-5
0
5
heatflux[W
/g]
temperature [C]
Zinc
endo
exo
TM
= 419.6 C
130 140 150 160 170 180-20
-15
-10
-5
0
5
H100%
= 28.45 J/g
TM
= 156.6 C
heatflux[W
/g]
temperature [C]
Indium
endo
ex
o
Calibration of Temperature and Heat Flux
ZincIndium
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Thermoanalytic Methods DTA/DSC
Application of DTA/DSC
Thermal transitions (e.g., glass transition, phase transitions) Melting behavior, -temperature, -enthalpy; specific heat
Crystallization behavior; recrystallization Degree of crystallinity
Annealing and curing processes; thermal stability
Desorption, evaporation, decomposition Efficiency of additives
Chemical reaction enthalpy, reaction temperature, reaction kinetics
7/31/2019 Characterization & Identification of Polymers Presentation
7/427To ic IV.1 & 2 Courtesy of University of Leoben, Austria
50 100 150 200
temperature [C]
1
0
PC film
50m
heatflux[W/g]
ex
o
endo
TG = 150C
Thermoanalytic Methods DTA/DSC
Amorphous Polymers Glass TransitionPolycarbonate (PC)
glass transition
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50 100 150
-11
-10
-9
-8
-7
-6
heatflux
[W/g]
temperature [C]
ABS/PC blend
e
xo
endo
Thermoanalytic Methods DTA/DSC
Amorphous Polymers Glass TransitionABS/PC blend
glass transition
ABSPC
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Thermoanalytic Methods DTA/DSC
Amorphous Polymers Glass Transition
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Thermoanalytic Methods DTA/DSC
Amorphous thermoplastics Glass transition temperature [C]
Polyvinylchloride (PVC) 80
Polystyrene (PS) 95
Polymethylmethacrylate (PMMA) 105
Polycarbonate (PC) 150
Polysulfone (PSU) 190
Polyethersulfone (PES) 230
Polyetherimide (PEI) 220
Athas Databank:http:web.utk.edu/~athas/databank/
Engineering and high temperature-resistant, amorphous polymers (PC, PSU, PES, PEI, etc.)contain aromatic rings, giving the macromolecule main chain a 2-dimensional (ladder-like) structure.
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Thermoanalytic Methods DTA/DSC
Semicrystalline Polymers Melting BehaviourPE-HD
60 80 100 120 140 160
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
TM
= 135C
heatflux
[W/g]
temperature [C]
PE-HDexo
endo
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Thermoanalytic Methods DTA/DSC
Semicrystalline Polymers Melting Behaviour
PE-HD and PE-LD
60 80 100 120 140 160
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
X
TM
= 115C
TM
= 135C
heatflux
[W/g]
temperature [C]
PE-HD
PE-LD
e
xo
endo
X
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Thermoanalytic Methods DTA/DSC
Semicrystalline Polymers Melting Behaviour
PE-LD / PP blend
40 60 80 100 120 140 160 180 200-1.1
-1.0
-0.9
-0.8
-0.7
-0.6
-0.5
-0.4
-0.3
heatflux
[W/g]
temperature [C]
PE-LD/PP Blend
exo
endo
XTM = 165C
TM
= 115C
X
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Thermoanalytic Methods DTA/DSC
Semicrystalline Polymers Melting Behaviour
w/o enthalpy relaxation
with enthalpy relaxation
Blend
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60 80 100 120 140 160
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
TM
= 135C
heatflux[W/g]
temperature [C]
PE-HDex
o
endo
X
60 80 100 120 140 160
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
heatflux[W/g]
temperature [C]
PE-HDex
o
endo
Melting Enthalpy (H) = 188 J/g
Thermoanalytic methods DTA/DSC
Semicrystalline Polymers Degree of Crystallinity
PE-HD
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Thermoanalytic Methods DTA/DSC
Semicrystalline Polymers Degree of Crystallinity
= H /H100%cr
... Degree of crystallinity
H ... Measured melting enthalpy
H100%cr ... Melting enthalpy for 100% crystalline material
Example PE-HD:
= 188/294 = 64%
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Thermoanalytic Methods DTA/DSC
Semicrystalline polymer Melting temperature[C]
Melting enthalpy for100% crystallinity [J/g]
Polyethylene (PE) 80 150
165
180
260
270
350
175
325
294
Polypropylene (PP) 207
Polyoxymethylene (POM) 326
Polyamide 6,6 (PA66) 270
Polyethyleneterephthalate (PET) 153
Polyether ether ketone (PEEK) 130
Poly(vinylidene fluoride) (PVDF) 105
Polytetrafluoroethylene (PTFE) 41
Athas Data bank:
http:web.utk.edu/~athas/databank/http://athas.prz.rzeszow.pl/databank/welcome-db.html
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Thermoanalytic Methods DTA/DSC
Semicrystalline Polymers Melting vs. Crystallization
PTFE
200 220 240 260 280 300 320 340 360-6
-4
-2
0
2
4
6 TCr
= 310 C
heatflux
[W/g]
temperature [C]
PTFEexo
endo
cooling, -10 K/min
heating, 10 K/min
TM
= 327C
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Thermoanalytic Methods DTA/DSC
Semicrystalline Polymers Postcrystallization
PET
50 100 150 200 250 300-20
-15
-10
-5
0
5
TM
= 250 C
TPostCr
= 150 C
heatflux
[W/g]
temperature [C]
quenched PET
endo
exo
TG
= 75 C
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Thermoanalytic Methods DTA/DSC
Polyolefines exhibit autooxidation. Oxidation temperature (TOx) is affected by stabilization and ageing.
weathering
50 100 150 200 250
2
0
unaged
weathered
PP film
heatflux[W/g]
temperature [C]
exo
endo
TOx
= 220 C
Degradation / Oxidation of Polymers - PP
Th l ti M th d DTA/DSC
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Thermoanalytic Methods DTA/DSC
Epoxy Resin - Relationship Between Degree of Cure
& Glass Transition Temperature
70 75 80 85 90 95 10060
80
100
120
140
160
180
200
220
epoxy resin
glasstrans
itiontempe
ratureT
gDS
C,
C
degree of cureDSC
, %
Th l ti M th d TGA
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Thermoanalytic Methods - TGA
Thermogravimetrical Analysis (TGA)
Sample (~10 mg) and crucible, connected to a microbalance, are placed in an oven. The oven is usually heated or cooled at a rate ranging between 0.1 and 100 K/min.
The change of weight (m) is measured as a function of temperature.
Th l ti M th d TGA
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Thermoanalytic Methods - TGA
Thermogravimetrical analysis (TGA)
0 100 200 300 400 50085
90
95
100
< 10 wt% phenolresin coating
temperature [C]
Phenol resin coated mineral wool
Relativemass[%]
< 2 wt% water content
Determination of volatile components (e.g., water, solvents, etc.) Determination of mineral filler or reinforcement content of plastics.
Topic IV:
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pStructural Characterization and Identification of Polymers
IV.1. Thermoanalytic methods- Differential thermal analysis (DTA) & differential scanning calorimetry (DSC)
- Thermogravimetric analysis (TGA)- Thermomechanical analysis (TMA)
IV.2. Spectroscopic methods
- IR Spectroscopy
IV.3. Microscopic methods- Optical/light Microscopy- Scanning Electron Microscopy
- Atomic force Microscopy
IV.4. Diffraction methods- X-Ray Diffraction
Spectroscopy
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Spectroscopy
Spectroscopic methods play an important role in structural analysis of polymers.
Spectroscopic phenomena are associated with the absorption or emission ofelectromagnetic radiation.
: wavelength
IR Spectroscopy
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IR - Spectroscopy
Infrared spectroscopy (IR)
For the analysis of plastics, infrared radiation with wavelength between2.5m and 25m is used.
For experimental reasons usually the wavenumber () is used instead of thewavelength ().
= 1/*10000 : wavenumber in cm-1 and
: wavelength in m
IR Spectroscopy
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IR - Spectroscopy
Infrared spectroscopy (IR)
The IR radiation causes rotations and vibrations of molecules and atomic groups. The oscillations are described by spring-mass-systems:
m2
m1
km1 : mass of group 1 (e.g., H, O, N, S, Cl, F, CH3 )
m2 : mass of group 2 (e.g., C, macromolecule)K : spring constant (e.g., C-H, C-O, C=O, C-N ...)
Absorption occurs when the exciting frequency is equal to the resonancefrequency of the system.
Due to the many different groups in polymers many different oscillations withspecific absorption peaks occur.
IR - Spectroscopy
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IR - Spectroscopy
Vibrations of CH2groups
C
HH
symmetric CHstretching vibration Antisymmetric CHstretching vibration H-C-H deformation(bending)
Rotation of CH2 group
(twisting)
Out-of plane pendulum vibration ofthe CH2 group (wagging)
In-plane pendulum vibrationof the CH2 group (rocking)
IR-Spectroscopy
IR - Spectroscopy
http://en.wikipedia.org/wiki/Infrared_spectroscopyhttp://en.wikipedia.org/wiki/Infrared_spectroscopy7/31/2019 Characterization & Identification of Polymers Presentation
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IR - Spectroscopy
Experimental IR-Spectrophotometer
Heatradiationsource
Interfero-meter
Detector,
Computer
Samplecompartment
IR-spectroscopy - PE
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IR spectroscopy PE
4 0 0 0 3 5 0 0 3 0 0 0 2 5 0 0 2 0 0 0 1 5 0 0 1 0 0 0
3 0
4 0
5 0
6 0
7 0
8 0
9 0
1 0 0
transmission[%]
w a v e n u m b e r [ c m-1
]
C H 2
Vibration Range
a CH2,s CH2 3000-2840
CH2 1471
CH2 717
* C C
H
H
*
H
H
n
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IR-spectroscopy - PS
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IR spectroscopy PS
4 0 0 0 3 5 0 0 3 0 0 0 2 5 0 0 2 0 0 0 1 5 0 0 1 0 0 0
3 0
4 0
5 0
6 0
7 0
8 0
9 0
1 0 0
transmissio
n[%]
w a v e n u m b e r [ c m - 1 ]
p h e n y l e n e
Vibration Range
=CH 3150-3000
a CH2,s CH2 3000-2840
Vibration Range
Ph 1600-1375
=CH 1067
=CH 1027
Vibration Range
=CH 906
=CH 754
Ph 695
* C
H
H
C *
H
n
IR-spectroscopy plasticized PVC
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IR spectroscopy plasticized PVC
4 0 0 0 3 5 0 0 3 0 0 0 2 5 0 0 2 0 0 0 1 5 0 0 1 0 0 0
7 0
7 5
8 0
8 5
9 0
9 5
1 0 0
transmis
sion[%]
w a v e n u m b e r [ c m - 1 ]
O H
Vibration Range
OH (plasticiser) 3331
a CH2, s CH2, CH 3000-2840
C(=O)C (plasticiser) 1720 CH2 1426
Vibration Range
CH, C-O-C (plast.) 1264
C-O (plast.) 1122, 1072
C-C 966 CH 742
* CH2 CH
Cl
*n
IR-spectroscopy PA12
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IR spectroscopy PA12
4 0 0 0 3 5 0 0 3 0 0 0 2 5 0 0 2 0 0 0 1 5 0 0 1 0 0 04 0
5 0
6 0
7 0
8 0
9 0
1 0 0
transmission[%]
w a v e n u m b e r [ c m - 1 ]
N H
C = O
N H , N C
C H 2
Vibration Range
NH 3287
a CH2 2918
s CH2 2850 C=O 1634
Vibration Range
NH, CN 1553, 1269
CH2 1465
CH2, CH2 1200 CH2 720
* C CH2O
NH *n
z
IR-spectroscopy - PET
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spect oscopy
4 0 0 0 3 5 0 0 3 0 0 0 2 5 0 0 2 0 0 0 1 5 0 0 1 0 0 00
2 0
4 0
6 0
8 0
1 0 0
transmiss
ion[%]
w a v e n u m b e r [ c m - 1 ]
O = Cp h e n y l e n e
Vibration Range
a CH2, s CH2 3000-2840
C=O 1713
Ph 1600-1325 C(=O)O, =CH 1242
Vibration Range
O-C, =CH 1095
=CH 1017
=CH 956, 873 Ph 725
* C
O
C O
O
CH2
CH2
O *n
IR-spectroscopy PTFE and ETFE
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p py
4 0 0 0 3 5 0 0 3 0 0 0 2 0 0 0 1 5 0 0 1 0 0 0
2 0
4 0
6 0
8 0
1 0 0
w a v e n u m b e r [ c m - 1 ]
transmission[%]
E T F E C - F C - C - F
2 0
4 0
6 0
8 0
1 0 0
transmission
[%]
P T F E
C F 2
PTFE: Vibration Range
a CF2 1200
s CF2 1145
ETFE: Vibration Range
a CH2, s CH2 3000-2840
CH 971
s CH2 1453, 1248, 1162
C-F 1323, 1038
CH2, C-C-F 666
* C C *
F
F
F
F
n
* C C C C
H
H H
H
*
F F
F F
n
IR-spectroscopy PES and PSU
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p py
4 0 0 0 3 5 0 0 3 0 0 0 2 0 0 0 1 5 0 0 1 0 0 0
8 0
8 5
9 0
9 5
1 0 0
transmission[%]
w a v e n u m b e r [ c m - 1 ]
P S U
6 0
7 0
8 0
9 0
1 0 0
transmission[%]
P E S
p h e n y l e n e
S O 2
Vibration Range
=CH 3086
a Me 1486
a Me, s Me 3000-2840
Ph 1600-1320
a SO2, =CH 1293, 1147
Vibration Range
a C-O-C 1233
=CH 833
=CH 1103
=CH, Me 1012
Ph 687
* O S *
O
O
n
* O C
CH3
CH3
O S
O
O
*n
IR-spectroscopy PEI and PI
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p py
4 0 0 0 3 5 0 0 3 0 0 0 2 0 0 0 1 5 0 0 1 0 0 08 89 0
9 2
9 4
9 6
9 8
1 0 0
w a v e n u m b e r [ c m - 1 ]
transm
ission[%]
P E IN C 2
9 2
9 4
9 6
9 8
1 0 0
transmission[%]
P I
i m i d e
Vibration Range
=CH 3150-3000
Ph 1600-1300
a Me & s Me (PEI) 3000-2840
a C=O, s C=O 1775, 1725
imide (PI) 1375
Vibration Range
imide, s Me (PEI) 1355
s C-O-C 1167, 1114, 1082
=CH (PI) 881, 821
C=O (PEI) 848
imide, aC-O-C (PI) 1243
s NC2 (PEI) 1236
C
C
O
N
C
C
O
N On
O O
C
C
O
O
N* O C
CH3
CH3
O
C
C
O
O
N
*n
IR-spectroscopy - EVA
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4 0 0 0 3 5 0 0 3 0 0 0 2 0 0 0 1 5 0 0 1 0 0 00
2 0
4 0
6 0
8 0
1 0 0
transmission[%]
w a v e n u m b e r [ c m - 1 ]
5 %
0
2 0
4 0
6 0
8 0
1 0 0
tr
ansmission[%]
2 4 %
Vibration Range
a CH2, s CH2 3000-2840
a CH3,s CH3 3000-2840
C=O 1740
CH2, a Me 1469
Vibration Range
s Me 1371
C(=O)O 1241
O-C, Me 1020
CH2 720
* CH2 CH *
O C CH3
O
n
IR-spectroscopy - EVA
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A = ln (0/)
Determination of Vinylacetate (VA) content
* C C
H
H
*
H
H
n
* CH2 CH *
O C CH3
O
n
Ethylene
A...Absorption
...transmission
Vinylacetate band:A(1240cm-1)...(C=O)O group
Ethylene band:
A(1472cm
-1
)...CH2, CH3 groups
5 10 15 20 25
Vinylacetate
0,5
1,0
1,5
2,0
2,5
3,0
3,5
4,0
A(1240cm-1
)/
A(1472cm
-1
)
VA [%]
y = 0,1427x + 0,038
R2
= 0,9646
IR-spectroscopy (ATR) - PE
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= 100% * [1-(Ia
/Ib
)/1.233]/(1+Ia
/Ib
)
Determination of PE-crystallinity
760 740 720 700 680
crystallinity value
Ia: Intensity peak area of the 730 cm-1 band
Ib: Intensity peak area of the 720 cm-1 band
1.233: area-ratio of pure crystalline polyethylene
720
Ib
- amorphous
absorptio
n[-]
wave number [cm-1]
730
Ia
- crystalline
IR-spectroscopy (ATR) - PE
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3 0 0 0 2 9 0 0 2 8 0 01 5 0 0 1 4 0 0 1 3 0 0 1 2 0 0 1 1 0 0 1 0 0 0 9 0 0 8 0 0 7 0 0
absor
ption[-]
w a v e n u m b e r [ c m - 1 ]
4 7 %
absorption[-] 8 1 %
* C C
H
H
*
H
H
n
Vibration Range
a CH2,s CH2 3000-2840
CH2 1500-1460
CH3 730-720