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Thermogravimetry

         Duncan Price
IPTME, Loughborough University
© Copyright: D.M.Price@lboro.ac.uk (2006)
definitions
“…. 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
programme.”



“Controlled temperature programme” can mean:
• heating and/or cooling at a linear rate (by far commonest)
• isothermal measurements
• combinations of heating, cooling and isothermal stages
• other, more modern approaches, in which the temperature
profile is modified according to the behaviour of the sample.
instrumentation
         GAS IN                                BALANCE
                                      WEIGHT
                                               CONTROLLER
GAS-TIGHT
ENCLOSURE

    SAMPLE




HEATER
                              SAMPLE TEMP.



           POWER          FURNACE TEMP.


                  TEMPERATURE PROGRAMMER
balance/furnace configurations
example curve




Mass (%) in green, rate of mass loss (%/°C) in blue.
physical limitations on the heating process
                          EXCHANGE OF GASES:
                          REACTING GASES IN,
                          PRODUCTS OUT


  CONVECTION
  THROUGH
  SURROUNDING
  ATMOSPHERE




                                        RADIATION FROM
                                        FURNACE WALL




  CONDUCTION
  THROUGH SAMPLE
  PAN AND
                                INDICATION OF SAMPLE
  INSTRUMENT
                                TEMPERATURE
factors that affect the results


A) INSTRUMENTAL                       B) SAMPLE-RELATED
• heating rate                        • mass
• furnace atmosphere and flow-rate    • particle size
• geometry of pan and furnace         • sample history/pre-treatment
• material of pan                     • packing
                                      • thermal conductivity
                                      • heat of reaction



 For a given instrument, careful standardisation of experimental
 procedures leads to highly reproducible results.
effect of heating rate




10 mg samples of PTFE, heated at 2.5, 5, 10 and 20 °C/min in nitrogen
isoconversion kinetic treatment
lifetime prediction
effect of atmosphere




CaC 2 CO 4 .H 2 O in air and nitrogen
sources of error
A) MASS                                     NOISY OR ERRATIC RECORDS
• Classical buoyancy                        CAN ARISE FROM:
• Effect temp. on balance                   • static
• convection and/or turbulence              • vibration
• viscous drag on suspension                • pressure pulses in lab.
These are lumped together as the “buoyancy”
                                               • uneven gas flow
correction, and if significant, can be allowed
for by a blank run



B) TEMPERATURE
Temperature calibration difficult to carry out accurately.
Many methods exist, but none totally satisfactory.
Best accuracy from simultaneous TG-DTA or TG-DSC instrument.
calibration
MASS - Use standard weights.
Use standard samples to check operation, but unwise to use them
as weight standards.
TEMPERATURE -
Four approaches:
• Observe deflection on Temperature/time curve
• Curie-point standards
• Drop-weight methods
• In simultaneous-type units, use melting standards
• DO NOT use decomposition events to define temperature.
calibration using sample thermocouple
calibration using drop weight
calibration using curie point
weight change/ mg


                    0.2



                                                 Nickel metal
                    0.0
                                                 3°C/min. in nitrogen




                                   350                  370
                                         temperature /°C
calibration using TG-DTA




10mg Gold (99.999%), 10°C/min, alumina pan, air.
polymer stability studies




a = PVC, b= nylon-6, c = LDPE, d= PTFE
compositional analysis of filled rubber
composition of PVAc
LDPE/nylon film
sample controlled TG
comparison of temperature programmes
modulated temperature thermogravimetry
thermogravimetry-EGA by mass
        spectroscopy
simultaneous DSC/DTA-thermogravimetry

                            R
               S




                   TR


                        T
                        Δ
simultaneous DSC-thermogravimetry
TGA-MS of PVC
thermogravimetry-EGA by FTIR
summary

  PROCESS                      WEIGHT GAIN   WEIGHT LOSS
Ad- or absorption                    

Desorption, drying                           
Dehydration, desolvation                     
Sublimation                                  
Vaporisation                                 
Decomposition                                
Solid-solid reactions (some)                 
Solid-gas reactions                         
Magnetic transitions                        
recommended reading


D. M. Price, D. J. Hourston & F. Dumont, “Thermogravimetry of Polymers”, R. A.
Meyers (Ed.), Encyclopedia of Analytical Chemistry, John Wiley & Sons Ltd.,
Chichester (2000) pp. 8094-8105.

G. R. Heal,”Thermogravimetry & Derivative Thermogravimetry”, in P.J. Haines (ed.)
Principles of Thermal Analysis & Calorimetry, ch. 4, Royal Society of Chemistry,
Cambridge (2002) pp. 10-54.

C. M. Earnest (Ed.), Compostional Analysis by Thermogravimetry, ASTM STP 97,
American Society for Testing and Materials (1988).

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Tga

  • 1. Thermogravimetry Duncan Price IPTME, Loughborough University © Copyright: D.M.Price@lboro.ac.uk (2006)
  • 2. definitions “…. 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 programme.” “Controlled temperature programme” can mean: • heating and/or cooling at a linear rate (by far commonest) • isothermal measurements • combinations of heating, cooling and isothermal stages • other, more modern approaches, in which the temperature profile is modified according to the behaviour of the sample.
  • 3. instrumentation GAS IN BALANCE WEIGHT CONTROLLER GAS-TIGHT ENCLOSURE SAMPLE HEATER SAMPLE TEMP. POWER FURNACE TEMP. TEMPERATURE PROGRAMMER
  • 5. example curve Mass (%) in green, rate of mass loss (%/°C) in blue.
  • 6. physical limitations on the heating process EXCHANGE OF GASES: REACTING GASES IN, PRODUCTS OUT CONVECTION THROUGH SURROUNDING ATMOSPHERE RADIATION FROM FURNACE WALL CONDUCTION THROUGH SAMPLE PAN AND INDICATION OF SAMPLE INSTRUMENT TEMPERATURE
  • 7. factors that affect the results A) INSTRUMENTAL B) SAMPLE-RELATED • heating rate • mass • furnace atmosphere and flow-rate • particle size • geometry of pan and furnace • sample history/pre-treatment • material of pan • packing • thermal conductivity • heat of reaction For a given instrument, careful standardisation of experimental procedures leads to highly reproducible results.
  • 8. effect of heating rate 10 mg samples of PTFE, heated at 2.5, 5, 10 and 20 °C/min in nitrogen
  • 11. effect of atmosphere CaC 2 CO 4 .H 2 O in air and nitrogen
  • 12. sources of error A) MASS NOISY OR ERRATIC RECORDS • Classical buoyancy CAN ARISE FROM: • Effect temp. on balance • static • convection and/or turbulence • vibration • viscous drag on suspension • pressure pulses in lab. These are lumped together as the “buoyancy” • uneven gas flow correction, and if significant, can be allowed for by a blank run B) TEMPERATURE Temperature calibration difficult to carry out accurately. Many methods exist, but none totally satisfactory. Best accuracy from simultaneous TG-DTA or TG-DSC instrument.
  • 13. calibration MASS - Use standard weights. Use standard samples to check operation, but unwise to use them as weight standards. TEMPERATURE - Four approaches: • Observe deflection on Temperature/time curve • Curie-point standards • Drop-weight methods • In simultaneous-type units, use melting standards • DO NOT use decomposition events to define temperature.
  • 14. calibration using sample thermocouple
  • 16. calibration using curie point weight change/ mg 0.2 Nickel metal 0.0 3°C/min. in nitrogen 350 370 temperature /°C
  • 17. calibration using TG-DTA 10mg Gold (99.999%), 10°C/min, alumina pan, air.
  • 18. polymer stability studies a = PVC, b= nylon-6, c = LDPE, d= PTFE
  • 19. compositional analysis of filled rubber
  • 30. summary PROCESS WEIGHT GAIN WEIGHT LOSS Ad- or absorption  Desorption, drying  Dehydration, desolvation  Sublimation  Vaporisation  Decomposition  Solid-solid reactions (some)  Solid-gas reactions   Magnetic transitions  
  • 31. recommended reading D. M. Price, D. J. Hourston & F. Dumont, “Thermogravimetry of Polymers”, R. A. Meyers (Ed.), Encyclopedia of Analytical Chemistry, John Wiley & Sons Ltd., Chichester (2000) pp. 8094-8105. G. R. Heal,”Thermogravimetry & Derivative Thermogravimetry”, in P.J. Haines (ed.) Principles of Thermal Analysis & Calorimetry, ch. 4, Royal Society of Chemistry, Cambridge (2002) pp. 10-54. C. M. Earnest (Ed.), Compostional Analysis by Thermogravimetry, ASTM STP 97, American Society for Testing and Materials (1988).

Editor's Notes

  1. Modulated temperature TG is a method for studying polymer degradation kinetics.This employs a temperature profile in which a sinusoidal temperature fluctuation is superimposed upon a conventional linear rising temperature program. The raw data from such an experiment are shown in on the left for an ethylene-co-vinyl acetate copolymer. The curves showing the heating rate (d T /d t ) and rate of mass loss (-d m /d t ) make the effect of the temperature modulations apparent. This data is used to calculate the activation energy for the thermal decomposition process in real time as shown on the right (from: D. M. Price, D. J. Hourston & F. Dumont, “Thermogravimetry of Polymers”, R. A. Meyers (Ed.), Encyclopedia of Analytical Chemistry. John Wiley & Sons Ltd., Chichester (2000) pp. 8094-8105).
  2. The most usual means of identification of evolved gases employs either infrared or mass spectrometry ) . In both cases, some form of interface is required to take the evolved gases from the thermobalance into the spectrometer. Mass spectrometry EGA is complicated by the requirement to operate the mass spectrometer under high vacuum. An example splitter design is shown above which is designed order to reduce the transfer line pressure down to a level suitable for injection into the mass spectrometer. These units are heated so as to prevent condensation of less volatile products. (from: S.B.Warrington in “Thermal Analysis - Techniques and Applications”, E.L.Charsley and S.B.Warrington, (eds.), Special Publication 117, Royal Society of Chemistry, Cambridge (1992)).
  3. DSC (or DTA) is another thermal analysis technique whereby the difference in heat flow (or temperature) between a sample and inert reference substance is measured during a temperature program. Any changes in heat capacity of the sample (such as accompanies the glass-rubber transition in polymers) or processes which consume (endothermic) or liberate (exothermic) heat can be studied. The sample is usually placed in an aluminium pan with an empty pan used as a reference. Various methods are used to measure the heat flux, but a common arrangement is to place the pans on a metal or ceramic plate containing thermocouples which serve to detect the difference in temperature between the pans and convert this to a thermal energy difference. Several instruments have been designed which incorporate the heat flux plate design into a thermobalance this affording a means of performing simultaneous DSC/DTA and TG. There are several advantages to this approach over conventional DSC and TG notwithstanding the saving in experimental time needed to acquire two sets of data. It is useful to be able to determine energy changes associated with thermal decomposition reactions. Because many chemical reactions in polymer systems, such as curing of thermosets, are condensation reactions, water or ammonia may be liberated during the course of the reaction. This will cause a change in mass of the sample in addition to the heat of reaction which can be measured by DSC. TG cannot normally detect physical changes in polymer structure such as those that accompany the glass transition, crystallisation or melting so the additional information provided by DSC is useful.
  4. An example of TG-DSC is shown above for a natural polymer (cellulose) containing an excess of water. The total moisture content of the polymer can be found from the mass loss on drying whereas the amount of free water can be determined from its enthalpy of fusion given by the area under the DSC peak around 0°C. The difference between the two values is the amount of water chemically bound to the polymer. This will vary for cellulose obtained from different sources and will influence its reactivity towards acids and alkalis. This can be important in the preparation of cellulose derivatives such as cellulose acetate (from: D. M. Price, D. J. Hourston & F. Dumont, “Thermogravimetry of Polymers”, R. A. Meyers (Ed.), Encyclopedia of Analytical Chemistry. John Wiley & Sons Ltd., Chichester (2000) pp. 8094-8105).
  5. A simple example of the application of thermogravimetry-mass spectrometry (TG-MS) to polymers is shown above which illustrates the effect of adding 4% added MoO 3 on the release of benzene (m/z =78) (a= pure polymer, b = polymer + additive).The reduction in the emission of benzene (m/z = 78) brought about by the incorporation of the additive is clearly evident (from: D. M. Price, D. J. Hourston & F. Dumont, “Thermogravimetry of Polymers”, R. A. Meyers (Ed.), Encyclopedia of Analytical Chemistry. John Wiley & Sons Ltd., Chichester (2000) pp. 8094-8105).
  6. FTIR is a useful alternative to MS as a means of evolved gas analysis. For thermogravimetry-infrared evolved gas analysis (TG-IR) the interface comprises a heated transfer line (to prevent the condensation of less volatile products) and a flow cell through which the beam from the spectrometer is passed. A TG is shown on the left for the mass loss and derivative mass loss profiles for plasticized cellulose acetate ) . The total signal from the infrared infrared detector is shown on the right along with a signal derived from the infrared absorbance of the plasticizer. Thus, infrared evolved gas analysis is a useful means of assigning multiple mass losses to specific degradation mechanisms (from: D. M. Price & S. P. Church, “FTIR Evolved Gas Analysis of the Decomposition Products of Cellulose Diacetate”, Thermochimica Acta, 294 (1997) 107-112).