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Dr. Anthony Brennan University of Florida Department of Materials Science Engineering

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Dr. Anthony Brennan University of Florida Department of Materials Science Engineering

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    1. EMA 6165 Polymer Physics AB Brennan 1 Dr. Anthony Brennan University of Florida Department of Materials Science & Engineering

    2. EMA 6165 Polymer Physics AB Brennan 2 Agenda Glass Transition values Organic Inorganic Thermodynamic Treatment of Tg Kinetics of Tg Physical Aging Behavior

    3. EMA 6165 Polymer Physics AB Brennan 3

    4. EMA 6165 Polymer Physics AB Brennan 4 Based in viscosity measurements of n-alkanes. Glass Transition Characteristics

    5. EMA 6165 Polymer Physics AB Brennan 5

    6. EMA 6165 Polymer Physics AB Brennan 6 = Fractional free volume @ Tg Glass Transition Characteristics

    7. EMA 6165 Polymer Physics AB Brennan 7 What are the factors to consider now:

    8. EMA 6165 Polymer Physics AB Brennan 8

    9. EMA 6165 Polymer Physics AB Brennan 9 Start lecture on FRIDAY April 20Start lecture on FRIDAY April 20

    10. EMA 6165 Polymer Physics AB Brennan 10 WLF

    11. EMA 6165 Polymer Physics AB Brennan 11

    12. EMA 6165 Polymer Physics AB Brennan 12 where Glass Transition Shift Factor

    13. EMA 6165 Polymer Physics AB Brennan 13 Normally Glass Transition Shift Factor

    14. EMA 6165 Polymer Physics AB Brennan 14 Thermodynamic Treatment

    15. EMA 6165 Polymer Physics AB Brennan 15 Ehrenfest 1st Order Transition Glass Transition Ehrenfest

    16. EMA 6165 Polymer Physics AB Brennan 16 2nd Order Glass Transition 2nd Order Transition

    17. EMA 6165 Polymer Physics AB Brennan 17 Glass Transition Characteristics

    18. EMA 6165 Polymer Physics AB Brennan 18 Consider Glass Transition Characteristics

    19. EMA 6165 Polymer Physics AB Brennan 19 and

    20. EMA 6165 Polymer Physics AB Brennan 20 Gibbs and Di Marzio

    21. EMA 6165 Polymer Physics AB Brennan 21 OR Glass Transition Isothermal Compressibility

    22. EMA 6165 Polymer Physics AB Brennan 22 Originally derived in terms of viscosity assuming:

    23. EMA 6165 Polymer Physics AB Brennan 23 Thus..... Glass Transition Characteristics

    24. EMA 6165 Polymer Physics AB Brennan 24 Time dependent quantity

    25. EMA 6165 Polymer Physics AB Brennan 25 Typically, Glass Transition Characteristics

    26. EMA 6165 Polymer Physics AB Brennan 26 Glass Transition Characteristics

    27. EMA 6165 Polymer Physics AB Brennan 27 Glass Transition Characteristics

    28. EMA 6165 Polymer Physics AB Brennan 28 Glass Transition Characteristics Kinetic Theory

    29. EMA 6165 Polymer Physics AB Brennan 29 Vh = Molar volume of hole Eh = Molar excess energy associated with hole Ej = Molar energy for disappearance of a hole Nh* = Equilbrium # of holes n = molar volume of segments No = moles of repeat units Glass Transition Characteristics

    30. EMA 6165 Polymer Physics AB Brennan 30 Relaxation time for the disappearance of a hole: Glass Transition Characteristics

    31. EMA 6165 Polymer Physics AB Brennan 31

    32. EMA 6165 Polymer Physics AB Brennan 32 Kovacs Apparent Activation Energy

    33. EMA 6165 Polymer Physics AB Brennan 33 Glass Transition Thermodynamic Approach

    34. EMA 6165 Polymer Physics AB Brennan 34 Partition function to define conformational states. Glass Transition Characteristics

    35. EMA 6165 Polymer Physics AB Brennan 35 Glass Transition Characteristics

    36. EMA 6165 Polymer Physics AB Brennan 36 Glass Transition Characteristics

    37. EMA 6165 Polymer Physics AB Brennan 37 Summary Glass Transition is a second order thermodynamic transition. Glass Transition is a fictive temperature dependent upon time, temperature, rate, pressure and thermal history. WLF equation describes behavior from above Tg to Tg-50C. Kinetics of Tg process appear Arrhenius.

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