Thermal Analysis An introduction
Transcript of Thermal Analysis An introduction
1
Thermal Analysis
An introduction
Ralf Franke NETZSCH Gerätebau GmbH, Selb 03.07.2005
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• Introduction
definition
information available
• Techniques and instruments
TG, DSC, STA, STA-MS, TG-FTIR, DIL, TMA, DMA,
• Visit of the NETZSCH Application laboratory
• Starting a DSC Measurement
• TG „Workshop“
Outline
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Definition (ASTM E 473-85):
Thermal Analysis is a group of techniques in which a
physical property of a substance is measured as a
function of temperature while the substance is
subjected to a controlled-temperature program.
(ICTA, 1980)
Thermal Analysis
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Temperature is one of the most frequently measured quantities.
Measurement with thermocouples or resistance thermometers.
Thermocouples for measuring temperature differences according to the
Seebeck effect:
If an electric conductor is exposed to a temperature gradient, an electron flow is generated inside the conductor, which causes an electromagnetic force (EMF, thermocouple voltage).
EMF = resulting voltage, S – Seebeck Coefficient.; t1 – temperature at the soldering joint, t2 – reference temperature
Temperature Measurement
soldering joint
Metal A
Metal B
EMF
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A suitable thermocouple can be formed by connecting two metal wires
with different thermal properties.
Seebeck coefficient for some selected materials (in µV/°C at 0°C)
Aluminium 3.5 Selenium 900
Cadmium 7.5 Silicon 440
Constantan (40% Ni + 60% Cu) –35 Silver 6.5
Copper 6.5 Tellurium 500
Germanium 300 Tungsten 7.5
Iron 19
Nickel-Chromium 25
Nickel –15
Platinum 0
Rhodium 6
Thermocouples
According to this list e.g. nickel-chromium and constantan (type E) would be a good combination.
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Thermocouple type
(+) Leg
(-) Leg
Generated emf change in µV/°C
(reference junction at 0°C)
approx. working temperature range
Notes
at 100°C
at 500°C
at 1000°C
K Ni-Cr (Chromel)
Ni-Al (Alumel)
42 43 39 0 …1100°C most suited for oxidising atmospheres
T Cu CuNi (Constantan)
46 - - -185 … 300°C excellent for low temperatures
J Fe CuNi 54 56 59 20 … 700°C used in reducing atmospheres as an unprotected thermocouple
N NiCrSi
(Nicrosil)
NiSi 30 38 39 0 … 1100°C very stable output signal at high temperatures
E NiCr CuNi 68 81 - -200 … 800°C highest thermal emf per °C
R Pt13Rh Platin-13%Rhodium
Platinum 8 11 13 0 … 1600°C high resistance to oxidation and corrosion
S Pt10Rh Platin-10%Rhodium
Platinum 8 9 11 0 … 1550°C similar characteristics to type R
B Pt30Rh Platin-30%Rhodium
Pt6Rh Platinum-6%Rhodium
1 5 9 0 ... 1600° similar characteristics to type R and S
Thermocouples according to ITS 90 and IEC 584-1
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ASTM E 473 – 85:
Thermogravimetry is a
technique in which the
mass of a substance is
measured as a function of
temperature while the
substance is subjected to
a controlled-temperature
program.
Thermogravimetry (TG)
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Thermogravimetry (TG)
gas outlet
sample
cooling
cooling
hoistsample carrier
balancegas inletprotective
gas inletpurge
relief valve
pressure sensor
cover support
sample carrier
vacuum
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Thermogravimetry (TG)
Some features:
• RT – 1000°C • resolution: 0.1 µg • vacuum-tight • autovac • ASC • TG-FTIR /TG-MS
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100.0 200.0 300.0 400.0 500.0 600.0 700.0 800.0 900.0Temperature /°C
40.00
50.00
60.00
70.00
80.00
90.00
100.00
TG /%
-12.26 %
-30.02 %
Residual Mass: 38.57 % (949.6 °C)
-19.15 %
Thermogravimetry (TG)
TG 209 Iris F1 sample mass: 10.12 mg crucible: Al2O3
atmosphere: air, 30 ml/min heating rate: 10 K/min
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and a reference materialis measured as a function of
temperature while the substance and reference is
subjected to a controlled-temperature program.
Differential Scanning Calorimetry (DSC)
reference sample
heat flow
temperature and heat flow sensor
thermal resistance
heating and cooling
ASTM E 473 – 85:
Differential Scanning
Calorimetry (DSC) is a
technique in which the
difference in energy
inputs into a substance
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Differential Scanning Calorimetry (DSC)
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Differential Scanning Calorimetry (DSC)
Exchangeable DSC Sensor Types
new t–Sensor
-180 ... 700°C
short response time silver sensor
m–Sensor
-150 ... 400°C
high sensitivity
silicon sensor
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Differential Scanning Calorimetry (DSC)
DSC 204 F1 Phoenix sample mass: 20.97 mg crucible: Al atmosphere: nitrogen 30 ml/min heating rate: 10 K/min
melting
cold crystallization glass transition
Heat flow
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STA: Principle
FurnaceRefer.Sam ple
DT
QPR
.
TG + DSC = STA
Thermogravimetry Differential Scanning Calorimetry
Simultaneous Thermal Analysis
TG, DSC applied to the same sample.
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TG (mass changes)- and DSC (caloric)-effects are measured on one sample in one run in one system. Comparability of results is ensured:
• no influence of material inhomogeneity • no influence of sample preparation • no influence of measurement conditions • faster measurement times
Advantages of STA method
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STA: Schematic Setup
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STA: Specifications
Top features of Netzsch STAs:
• -160 ... 2000°C • resolution: 0.1 µg • vacuum-tight • low drift (~mg/h) • coupling with MS/FTIR
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STA: Application
Dehydration:
Montmorillonit Montmorillonit
Böhmit Diaspor & Hydrargillit
Kaolinit
Decomposition
of CaCO3
burn-up of organics
STA 409 PC sample mass: 52.46 mg crucible: Pt
atmosphere: air, 75 ml/min heating rate: 10 K/min
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STA is a powerful tool, however ...
... no direct chemical identification of the evolved gases and thus of the sample!
EGA using MS and FTIR !
Add-on: Monitoring of the partial pressures of the sample atmosphere (consumption of gas?)!
STA-MS
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STA-MS
NETZSCH Skimmer ®
+ STA 409 CD
NETZSCH QMS 403 C Aëolos ® + STA 449 Jupiter ®
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Simultaneous measuring of STA, MS and FTIR!
Consequent heating of the entire coupling interface (up to 300°C)!
prevention of condensation of evolved gases
enhance the traceability of evolved gases
minimize the risk of blocking of the coupling capillary
STA-MS: Capillary Coupling (Aëolos®)
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STA-MS-interface within furnace!
Best prevention of condensation of evolved gases
enhanced sensitivity compared to capillary coupling
STA-MS: Skimmer® Coupling
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STA-MS: Application
STA 449 C + Aëolos mass: 29.53 mg crucible: Pt
atmosphere: Ar, 50 ml/min heating rate: 10 K/min
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STA-MS: Application
STA 449 C + Aëolos mass: 29.53 mg crucible: Pt
atmosphere: Ar, 50 ml/min heating rate: 10 K/min
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TG-FTIR-MS
BRUKER
TENSORTM27 NETZSCH
TG 209C F1 IRIS®
NETZSCH QMS Aeolos®
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TG-FTIR
FTIR gas cell
(230°C)
transfer line
(230°C)
control
thermocouple adaptor head
(230 °C)
control
thermocouple
micro furnace
sample
sample carrier
control
thermocouple
IR detector
TG cell
gas outlet
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100 200 300 400 500 600 700 800 900Temperature /°C
30
40
50
60
70
80
90
100
TG /%
0
0.05
0.10
0.15
0.20
Gram Schmidt
-6.0
-5.0
-4.0
-3.0
-2.0
-1.0
0
1.0
DTG /(%/min)
-12.05 %
-18.81 %
-29.48 %
TG-FTIR
TG 209 Iris F1 - FTIR sample mass: 10.12 mg crucible: Al2O3
atmosphere: air, 30 ml/min heating rate: 10 K/min
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TG-FTIR
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F:\measurement\2004\001-3-04\001-3-04-02\490.0 CaC2O4_air_1 10.120 | NETZSCH TG 209 | F:\measurement\2004\CaC2O4\001-3-04-02.dt2
F:\measurement\0_libspectra\CO.01 CARBON MONOXIDE
F:\measurement\0_libspectra\CO2.01 CARBON DIOXIDE
1000150020002500300035004000
Wavenumber cm-1
0.0
0.5
1.0
1.5
2.0
2.5
Absorb
ance U
nits
TG-FTIR
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Dilatometry (DIL)
A technique in which a dimension of a substance under negligible load is measured as a function of temperature while the substance is subjected to a controlled temperature program.
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Dilatometry (DIL)
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Dilatometry (DIL)
Some features: • -260°C – 2800°C • vaccum-tight • inert, oxdizing and reducing atmospheres • up to 0.125 nm/digit resolution for 500 µm range • solids, pastes, powders, molten metals • Dil-MS and Dil-FT-IR
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Dilatometry (DIL)
Dil Application Example
Dil 402 C Sample: Quartz Crystal Sample holder: fused silica Heating rate: 2 Kmin Atmosphere: Helium
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Thermomechanical Analysis (TMA)
TMA – Thermomechanical-Analysis A technique in which the deformation of a substance under non-oscillatory load is measured as a function of temperature while the substance is subjected to a controlled temperature program.
DIN 51005; ASTM E 831
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Thermomechanical Analysis (TMA)
TMA – Thermomechanical-Analysis
TMA 202 TMA 402
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Thermomechanical Analysis (TMA)
TMA – Thermomechanical-Analysis
TMA 202
Some features: • -150°C –600°C • heating rates up to 50 K/min • sensitivity: 1 dig./1.25 nm • load: 0.01 to 1 N
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Thermomechanical Analysis (TMA)
TMA Application Example
TMA 202 Sample: PMMA Mode: Exansion Sample length: ~1.8 mm Sample holder: Fused Silica Heating rate: 10 K/min Atmosphere: Air
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Dynamic Mechanical-Analysis (DMA)
Determination of the mechanical properties of a sample
under an oscillating load and as a function of temperature,
time and frequency
DMA - Dynamic Mechanical Analysis
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Dynamic Mechanical-Analysis (DMA)
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Dynamic Mechanical-Analysis (DMA)
Some features:
• 8 N static and ± 8 N dynamic force • frequency range: 0.01 - 100 Hz • modulus range E´: 10-3 – 106 MPa • tan range: 0.00006 to 10 • -170°C – 600°C • heating rate: 0.1 – 20 K/min
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Dynamic Mechanical-Analysis (DMA)
DMA Measuring Modes
Shear
Tension 3-Point Bending
Compression / Penetration
Single/Dual Cantilever
Prestress (Static) Oscillation Sample
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Dynamic Mechanical-Analysis (DMA)
DMA Application Example
-80 -60 -40 -20 0 20 Temperature /°C
0.000
0.200
0.400
0.600
0.800
1.000
tan d
500.0
1000.0
1500.0
2000.0
2500.0
3000.0
3500.0
4000.0
4500.0
E' /MPa
0
200
400
600
800
1000
E'' /MPa
1.00 Hz
2.00 Hz
5.00 Hz
10.00 Hz
Rubber
Peak: -59 °C, 0 .806
Onset: -70 °C, 4679 .3 MPa
Peak: -64 °C, 880 .4 MPa
DMA 242 C sample holder: single cantilever 16 mm amplitude: ± 40 µm
atmosphere: static air heating rate: 2 K/min
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A low voltage AC signal (input)
is applied at one electrode
The response signal detected
at the other electrode (output)
is attenuated and phase shifted
Fundamental Principle of DEA ASTM E 2038 and E 2039
Dielectric Sensor: • Alignment of dipoles • Mobility of ions
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The NETZSCH DEA Series for Cure Monitoring of Reactive Resins
Dielectric Analysis (DEA)
– DEA 230 for most thermosets, adhesives, paints and coatings
– DEA 231 for fast curing resins as SMC/BMC and UV curing
– DEA 234 CurePak™ for continous processes
– MiniPress MPS 235
Implantable (disposable) sensors
Robust and reusable sensors
Surface (fringing field) or bulk measurements
For laboratory tests and curing in process (ovens, molds, presses)
Multi-channel instruments available
for DEA signal and temperature
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PARALLEL PLATE
ELECTRODES
COMB ELECTRODES INTERDIGITAL
CO-PLANAR
BULK FIELD FRINGE FIELD
POLYMER
DEA Sensor Geometry and Types
Monotrode Sensor in Spring Mold Tool Mount Sensor
Micron Sensor
IDEX Sensor
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Ion Viscosity and Loss Factor for the Flowing and Curing of an Epoxy Resin
lowest viscosity
best flow
highest viscosity
end of curing
+
+
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Buoyancy Effect for STA/TG Measurements Workshop
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Buoyancy:
The sample „swims“ in
the atmosphere. The
buoyancy (Archimedes
principle) becomes
smaller with increasing
temperature; as a
consequence the
balance shows an
apparent mass increase.
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Buoyancy and Convection - 1
Depending on
Atmosphere
Type of the sample carrier
Heating rate
Crucible volume
Fa = g • ρ • VK
ΔFa = g • VK • (ρ1- ρ2)
Ar
N2
He
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Buoyancy and Convection - 2
100 200 300 400 500 600 700 800 900Temperature /°C
-0.30
-0.20
-0.10
-0.0
0.10
0.20
0.30
0.40
TG /mg
Depending on
Atmosphere
Type of the sample carrier
Heating rate
Crucible volume
20 K/min
2.5 K/min 10 K/min
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Buoyancy and Convection - 3
Depending on
Atmosphere
Type of the sample carrier
Heating rate
Crucible volume
For large sample masses
(big crucible volume) it is
recommended to carry out
the correction curve with an
inert material (e.g. Al2O3).
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100 200 300 400 500 600Temperatur /°C
0
0.100
0.200
0.300
0.400
0.500
0.600
0.700
0.800
0.900
TG /mg
DTA/Al2O3-Tiegel
DSC/Pt-Tiegel
Buoyancy and Convection - 4
Depending on
Atmosphere
Type of the sample carrier
Heating rate
Crucible volume
DTA/Al2O3 crucibles
DSC Pt crucibles
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Buoyancy and Convection - 5
Ca oxalate measurement
without correction
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Buoyancy and Convection - 6
TG/DSC measurement
in Pt crucibles,
Sample mass: 24.69 mg
Ca oxalate measurement
with correction
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Mass Calibration - 1
Method 1:
Taking the recommendation from DIN 51 006 into consideration
- Call up the calibration mode of the instrument (if available)
- Put on one or several standard weights at room temperature
(in case of STA 409 PC Luxx this will be done automatically)
- compare the displayed mass with the nominal one
Method 2: Using Calcium Oxalat Monohydrate
- Calciumoxalat Monohydrat shows between room temperature and
950°C three well separated mass loss steps
- Compare the experimental mass loss values (corrected curve) with
the nominal ones
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Mass Calibration - 2
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Mass Calibration - 3
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Example: Calculation of theretical mass loss steps
Molecular weights:
Ca = 40 g/mol; C= 12 g/mol; O2 = 32 g/mol, H2 = 2g/mol,
C02 = 44 g/mol, CO = 28 g/mol
1) 146 g/mol to 128 g/mol = (18/146) = mass loss 12.4%
2) 128 g/mol to 100 g/mol = (28/146) = mass loss = 19.1%
3) 100 g/mol to 56 g/mol = (44/146) = mass loss = 30.1 %
All calculations have to be related to the starting mass of CaC2O4 x H20
(146 g/mol)
Mass Calibration - 4