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Byeong-Joo Lee POSTECH - MSE calphad@postech.ac.kr

Microstructure Evolution. Basic Review of Thermodynamics. Byeong-Joo Lee POSTECH - MSE calphad@postech.ac.kr. Objective. Understanding and Utilizing Thermodynamic Laws State function Thermodynamic Laws Statistical thermodynamics Gibbs energy Extension of Thermodynamics

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Byeong-Joo Lee POSTECH - MSE calphad@postech.ac.kr

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  1. Microstructure Evolution • BasicReviewof • Thermodynamics Byeong-Joo Lee POSTECH - MSE calphad@postech.ac.kr

  2. Objective • Understanding and Utilizing Thermodynamic Laws • State function • Thermodynamic Laws • Statistical thermodynamics • Gibbs energy • Extension of Thermodynamics • Multi-Phase System • Multi-Component System • Partial Molar Quantities • Utilization of Thermodynamics • Phase Diagrams • Defect Thermodynamics

  3. 1-2.Extensionof Thermodynamics • Multi-Phase System • Multi-Component System • Partial Molar Quantities

  4. Phase Diagram for H2O

  5. Phase Diagram for Fe

  6. Phase Diagram for Fe

  7. Equilibrium • Thermal, Mechanical and Chemical Equilibrium • Concept of Chemical Potential • In a one component system, • Temperature and Pressure dependence of Gibbs free energy

  8. Temperature Dependence of Gibbs Energy

  9. Temperature Dependence of Gibbs Energy - for H2O

  10. Temperature & Pressure Dependence of Gibbs Energy • Clausius-Clapeyron equation • For equilibrium between the vapor phase and a condensed phase constant constant

  11. Phase Diagram - for H2O • for S/L equilibrium

  12. Equilibrium vapor pressures vs. Temperature

  13. Equilibrium vapor pressures vs. Temperature

  14. Example - Phase Transformation of Graphite to Diamond • Calculate graphite→diamond transformation pressure at 298 K, given • H298,gra – H298,dia = -1900 J • S298,gra = 5.74 J/K • S298,dia = 2.37 J/K • density of graphite at 298 K = 2.22 g/cm3 • density of diamond at 298 K = 3.515 g/cm3

  15. 1-2.Extensionof Thermodynamics • Multi-Phase System • Multi-Component System • Partial Molar Quantities SolutionThermodynamics

  16. Thermodynamic Properties of Gases - mixture of ideal gases 1 mole of ideal gas @ constant T: • Mixture of Ideal Gases • Definition of Mole fraction: xi • Definition of partial pressure: pi • Partial molar quantities:

  17. Thermodynamic Properties of Gases - mixture of ideal gases Heat of Mixing of Ideal Gases Gibbs Free Energy of Mixing of Ideal Gases Entropy of Mixing of Ideal Gases

  18. Thermodynamic Properties of Gases - Treatment of nonideal gases Introduction of fugacity, f as For Equation of state ※ actual pressure of the gas is the geometric mean of the fugacity and the ideal P ※ The percentage error involved in assuming the fugacity to be equal to the pressure is the same as the percentage departure from the ideal gas law

  19. Thermodynamic Properties of Gases - Treatment of nonideal gases Alternatively, Example) Difference between the Gibbs energy at P=150 atm and P=1 atm for 1 mole of nitrogen at 0 oC

  20. Solution Thermodynamics - Mixture of Condensed Phases Vapor A: oPA Condensed Phase A Vapor B: oPB Condensed Phase B Vapor A+ B: PA + PB Condensed Phase A + B + → for gas

  21. Solution Thermodynamics - ideal vs. non-ideal solution Ideal Solution Nonideal Solution

  22. Solution Thermodynamics - Thermodynamic Activity Thermodynamic Activity of a Component in Solution → for ideal solution Draw a composition-activity curve for an ideal and non-ideal solution Henrian vs.Raoultian

  23. Solution Thermodynamics - Partial Molar Property ▷ Partial Molar Quantity ▷ Molar Properties of Mixture Gibbs-Duhem Equation

  24. Solution Thermodynamics - Partial Molar Quantity of Mixing definition of solution and mechanical mixing where is a pure state value per mole whyuse partial molar quantity?

  25. Solution Thermodynamics - Partial Molar Quantities

  26. Solution Thermodynamics - Partial Molar Quantities • Evaluation of Partial Molar Properties in 1-2 Binary System • Partial Molar Properties from Total Properties example) • Partial molar & Molar Gibbs energy • Gibbs energy of mixing vs. Gibbs energy of formation • Graphical Determination of Partial Molar Properties: Tangential Intercepts • Evaluation of a PMP of one component from measured values of a PMP • of the other example)

  27. Solution Thermodynamics - Non-Ideal Solution ▷ Activity Coefficient ▷ Behavior of Dilute Solutions

  28. Solution Thermodynamics - Quasi-Chemical Model, Guggenheim, 1935.

  29. Solution Thermodynamics - Regular Solution Model Sn-In Sn-Bi

  30. Solution Thermodynamics - Sub-Regular Solution Model Sn-Zn Fe-Ni

  31. Solution Thermodynamics - Regular Solution Model • Composition and temperature dependence of Ω • Extension into ternary and multi-component system • Inherent Inconsistency • Advanced Model → Sublattice Model

  32. Solution Thermodynamics - AdvancedGibbs Energy Model

  33. Summary - Gibbs Energy, ChemicalPotential and Activity ▷ Gibbs energy of mixing vs. Gibbs energy of formation ▷activity wrt. liquid A or B ▷ activity wrt. “ref” A or B ▷ activity wrt. [ ] i ▷ activity wrt. [ ] i

  34. Example • What is the difference between Gibbs energy of formation • andGibbs energy of mixing? • 2. What do Henrian behavior and Raoultian behavior mean for • a solution? Consider an A-B binary solution phase. • Show that each component shows aHenrian behavior • in dilute region and a Raoultian behavior in rich region, • if the molar Gibbs energy is expressed as follows.

  35. 1-3.Utilizationof Thermodynamics • PhaseDiagrams • Defect Thermodynamics

  36. Propertyof a Regular Solution

  37. Propertyof a Regular Solution

  38. Standard States

  39. Standard States

  40. Standard States Which standard states shall we use?

  41. Phase Diagrams- Relation with Gibbs Energy of Solution Phases

  42. Phase Diagrams- Binary Systems

  43. Phase Equilibrium 1. Conditions for equilibrium 2. Gibbs Phase Rule 3. How to interpret Binary and Ternary Phase Diagrams ▷ Lever-Rule

  44. Gibbs energy of ternary alloys

  45. 1-3.Utilization of Thermodynamics • PhaseDiagrams • Defect Thermodynamics • - Size Effect

  46. Introduction- Melting Point Depression of Nano Particles Au In M. Zhang et al. Phy. Rev. B 62 (2000) 10548. Sn S.L. Lai et al., Phys. Rev. Lett. 77 (1996) 99.

  47. Introduction - VLS Growth of Nanowires

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