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Thermodynamics Basic Review of Byeong-Joo Lee Microstructure Evolution

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Presentation on theme: "Thermodynamics Basic Review of Byeong-Joo Lee Microstructure Evolution"— Presentation transcript:

1 Thermodynamics Basic Review of Byeong-Joo Lee Microstructure Evolution
POSTECH - MSE

2 Understanding and Utilizing Thermodynamic Laws
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 Multi-Phase System Multi-Component System Partial Molar Quantities
1-2. Extension of 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 = 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 = g/cm3

15 Multi-Component System Partial Molar Quantities
1-2. Extension of Thermodynamics Multi-Phase System Multi-Component System Partial Molar Quantities Solution Thermodynamics

16 Thermodynamic Properties of Gases - mixture of ideal gases
1 mole of ideal 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

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 why use 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 - Advanced Gibbs Energy Model

33 Summary - Gibbs Energy, Chemical Potential 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
and Gibbs 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 a Henrian behavior in dilute region and a Raoultian behavior in rich region, if the molar Gibbs energy is expressed as follows.

35 Phase Diagrams Defect Thermodynamics
1-3. Utilization of Thermodynamics Phase Diagrams Defect Thermodynamics

36 Property of a Regular Solution

37 Property of a Regular Solution

38 Standard States

39 Standard States

40 Standard States Which standard states shall we use?

41

42

43

44 Phase Diagrams - Relation with Gibbs Energy of Solution Phases

45 Phase Diagrams - Binary Systems

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

47 Gibbs energy of ternary alloys

48 Defect Thermodynamics - Size Effect
1-3. Utilization of Thermodynamics Phase Diagrams Defect Thermodynamics - Size Effect

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

50 Introduction - VLS Growth of Nanowires

51 Interface Energy - Curvature effect

52 Curvature Effect – Capillary Pressure
System condition T = constant Vα = Vβ = V = constant @ equilibrium

53 Curvature Effect – on Vapor Pressure and Solubility
Solubility of pure B phase in a dilute solution

54 Curvature Effect – Capillary Pressure Effect on Melting Point - 1
M. Zhang et al. Phy. Rev. B 62 (2000)

55 Curvature Effect – Capillary Pressure Effect on Melting Point - 2

56 Curvature Effect – Capillary Pressure Effect on Melting Point - 2

57 Size dependence of SiGe nanowire composition – an example
I. Sa et. al., CALPHAD (2008)


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