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Phase Transformations. Growth Kinetics. Byeong-Joo Lee POSTECH-MSE. General Background. ※ References: 1. W.D. Kingery, H.K. Bowen and D.R. Uhlmann, "Introduction to Ceramics", John Wiley & Sons. Chap. 8. 2. Christian, section 56 & 54.
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Phase Transformations Growth Kinetics Byeong-Joo LeePOSTECH-MSE
General Background ※ References: 1. W.D. Kingery, H.K. Bowen and D.R. Uhlmann, "Introduction to Ceramics", John Wiley & Sons. Chap. 8. 2. Christian, section 56 & 54. 3. J. Burke, "The Kinetics of Phase Transformations in Metals," Pergamon Press. Chap. 6.
General Background • Nucleation vs. Growth • Crystal Growth vs. Grain Growth vs. Precipitate Growth • Driving force • Rate Determining Step • Parallel process vs. Serial Process
Classification of Growth Process - Interface-Reaction Controlled Growth □Interface-Reaction Controlled Growth ▷ Changes which do not involve long-range diffusional transport ex) growth of a pure solid grain growth - curvature driven kinetics recrystallization massive transformation martensitic transformation antiphase domain coarsening order-disorder transformation ※ Even phase transformations that involve composition changes may be interface-reaction limited. - local equilibrium is not applied at the interface.
Classification of Growth Process - Diffusion Controlled Growth □Diffusion Controlled Growth ▷ Changes which involve long-range diffusional transport ▷ Assumptions ․ local equilibrium at the interface : the concentration on either side of the interface is given by the phase diagram ※ for conditions under which this assumption might break down, see: Langer & Sekerka, Acta Metall. 23, 1225 (1975). ․ capillarity effects are ignored. ․ the diffusion coefficient is frequently assumed to be independent from concentration.
Interface-Reaction Controlled Growth - Mechanism □ Two types of IRC growth mechanism - Continuous growth and growth by a lateral migration of steps Continuous growth can only occur when the boundary is unstable with respect to motion normal to itself. - It can add material across the interface at all points with equal ease. - Comparison of the two mechanisms Continuous GrowthLateral motion of steps disordered interface ordered/singular interface diffuse interface sharp interface high driving force low driving force
Interface-Reaction Controlled Growth - Growth of a pure Solid ex) single crystal growth during solidification or deposition ▷ Continuous growth reaction rate in a thermally activated process (in Chemical Reaction Kinetics) ⇒ (ν/RT)·exp (-ΔG*/RT)·ΔGdf a thermally activated migration of grain boundaries ⇒ v = M·ΔGdf for example, for solidification ⇒ v = k1․ΔTi
Interface-Reaction Controlled Growth - Growth of a pure Solid ▷ Lateral growth ex) solidification of materials with a high entropy of melting minimum free energy ⇔ minimum number of broken bond source of ledge of jog : (i) surface nucleation (ii) spiral growth (iii) twin boundary (i) surface nucleation : two-dimensional homogeneous nucleation problem existence of critical nucleus size, r* the growth rate normal to the interface ∝ nucleation rate ⇒ v ∝ exp ( - k2 /ΔTi) (ii) spiral growth : ⇒ v = k3·(ΔTi)2 (iii) twin boundary : similar to the spiral growth mechanism
Interface-Reaction Controlled Growth - Growth of a pure Solid ▷ Heat Flow and Interface Stability (for pure metal) In pure metals solidification is controlled by the conduction rate of the latent heat. Consider solid growing at a velocity v with a planar interface into a superheated liquid. Heat flux balance equation KsT's = KLT'L + v Lv when T'L < 0, planar interface becomes unstable and dendrite forms. Consider the tip of growing dendrite and assume the solid is isothermal (T's = 0). T'L is approximately given by ΔTc/r
Interface-Reaction Controlled Growth - Grain growth in polycrystalline solids ▷ Capillary Effect Consider arbitrarily curved surface element · system condition : Vα=Vβ= V = const. T = const. · dF = -S dT - P dV + γdA = - Pβ dVβ - Pα dVα + γdA = - (Pβ - Pα) dVβ + γdA @ equilibrium - (Pβ - Pα) dVβ + γdA = 0 ∴ dA = (r1 + δr) θ1․(r2 + δr) θ2 - r1 θ1․r2 θ2 = (r1 + r2) δr θ1θ2 + (δr)2θ1 θ2 ≈ (r1 + r2) δr θ1θ2 dVβ 〓 r1r2θ1θ2 δr
Interface-Reaction Controlled Growth - Grain growth in polycrystalline solids ▷ Reaction rate · jump frequency νβα = νo exp(-ΔG*/RT) ναβ = νo exp(-[ΔG*+ΔGdf]/RT) ⇒ νnet = ν = νo exp(-ΔG*/RT) (1 - exp(-ΔGdf/RT)) if ΔGdf << RT ∴ ν 〓 νo exp(-ΔG*/RT)·ΔGdf/ RT ▷ Growth rate, u u = λν ; λ - jump distance
Interface-Reaction Controlled Growth - Grain growth in polycrystalline solids ▶ Grain Growth - no composition change & no phase (crystal structure) change - capillary pressure is the only source of driving force · α and β is the same phase · ∴ : normal growth equation ※ Role of Mobility / Role of Anisotropy in Grain boundary Energy 1. "Grain Growth Behavior in the System of Anisotropic Grain Boundary Mobility," Nong Moon Hwang, Scripta Materialia 37, 1637-1642 (1997). 2. "Texture Evolution by Grain Growth in the System of Anisotropic Grain Boundary Energy," Nong Moon Hwang, B.-J. Lee and C.H. Han, Scripta Materialia 37, 1761-1767 (1997).
Interface-Reaction Controlled Growth - Grain growth in polycrystalline solids ▶ Recrystallization (primary) - no composition change & no phase (crystal structure) change - stored strain energy is the main source of driving force · α and β is the same phase, but α has higher energy (strain energy) ※ Correlation between Deformation Texture and Recrystallization Texture 1. "The evolution of recrystallization textures from deformation textures," Dong Nyung Lee Scripta Metallurgica et Materialia, 32(10), 1689-1694, 1995 2. "Maximum energy release theory for recrystallization textures," Dong Nyung Lee Metals and Materials 2(3), 121-131, 1996.
Interface-Reaction Controlled Growth - Grain growth in polycrystalline solids ▶ Phase Transformations - no composition change & phase (crystal structure) change - Gibbs energy difference is the main source of driving force - ex) Massive transformation in alloys, Polymorphism ※ Linear relationship between interfacial velocity and driving force are common but not the rule.
Diffusion Controlled Growth - Precipitate Growth ※ As a thermally activated process with a parabolic growth law ·v ∝ ΔXo ·x ∝ t 1/2
Diffusion Controlled Growth - Lengthening of Needles (spherical tip)
Diffusion Controlled Growth - Growth of a lamella eutectic/eutectoid ※ Exactly the same results can be obtained when considering capillarity effectat the tip of each layer
Diffusion Controlled Growth - Growth of a lamella eutectic/eutectoid
Diffusion Controlled Growth - Growth of a lamella eutectic/eutectoid
Diffusion Controlled Growth - Growth of a lamella eutectic/eutectoid
Diffusion Controlled Growth - Growth of a lamella eutectic/eutectoid ∴ by examining the dependence of growth rate on S, one can see which one of the two diffusion mechanisms is more important.
Diffusion Controlled Growth - Coarsening of Precipitates (Ostwald ripening)
Diffusion Controlled Growth - Coarsening of Precipitates (Ostwald ripening)
Diffusion Controlled Growth - Coarsening of Precipitates (Ostwald ripening)
Diffusion Controlled Growth - Coarsening of Precipitates (Ostwald ripening)