EMA5001 Lecture 14 Growth of Alloys from Liquid © 2016 by Zhe Cheng Solidification of Single Phase Alloys (1) Most commercial metals contain alloy elements Systems to be examined T T1 T2 T3 TE Single phase Eutectic alloy Peritectic alloy Case #1 Equilibrium solidification of single phase alloys Assuming straight solidus and liquidus lines Infinitely slow cooling Liquid and solid phase uniform Average liquid composition follow liquidus line Average solid composition follows solidus line EMA 5001 Physical Properties of Materials XS XL k Zhe Cheng (2016) XL XS kX0 Solid X0 X0/k XB XL X0 XB Liquid XS Interface movement 14 Alloy Solidification x 2 Solidification of Single Phase Alloys (2) Case #2 No diffusion in solid, perfect mixing in liquid T Example Fast cooling with efficient stirring in liquid T1 Uniform liquid composition at any time T2 T3 Local equilibrium at the solid-liquid TE interface Liquid composition follow liquidus line Solid composition changes with position as a result of solidification at decreasing temperature with no diffusion in solid Average solid composition lower (in solute concentration) than solidus line Always reaches eutectic point EMA 5001 Physical Properties of Materials Zhe Cheng (2016) k XS XS XL XL XS kX0 X0 14 Alloy Solidification X0/k XE XB 3 Solidification of Single Phase Alloys (3) T Continue from p.3 Evolution of composition profile k Initial T T1 XB T1 T2 T3 TE Liquid X0 kX0 XS XS kX0 T1 < T = T2 < TE XB Liquid Solid X0 kX0 XL x Solid XB XS XL XL XS x EMA 5001 Physical Properties of Materials X0 Xmax X0/k XE XB Final T TE Solid Xmax X0 kX0 Zhe Cheng (2016) XE x 14 Alloy Solidification 4 Solidification of Single Phase Alloys (4) Continue from p.4 At any given extent of solidification XL Liquid composition (uniform) XL+dXL XL XB Solid Liquid XS Solid composition at the interface X0 XS fS Total weight fraction of solid kX0 fL=1-fS Total weight fraction of liquid fS fS+dfS dfS Small increase in solid weight fraction due to continued solidification dXL Small increase in liquid composition due to solute diffusion from solid to liquid df S dX L We have: X L X S df S 1 f S dX L 1 fS X L X S Consider k X S , we have df 1 dX S L XL fL 1 k X S kX 0 X0 Integral and consider when fS = 0, XS = kX0 , we have X S X 1 k L 1 k 1 f f S L Implication: the system will always contain some eutectics EMA 5001 Physical Properties of Materials Zhe Cheng (2016) 14 Alloy Solidification 5 Solidification of Single Phase Alloys (5) Case #3 No diffusion in solid, diffusional mixing in liquid T Assumption: T1 After initial stage, system can reach XS T2 steady state with stable solidification T3 rate TE Liquid composition decreases from liquidus line to bulk concentration Local equilibrium at the solid-liquid interface kX0 X0 System can reaches steady state: balance of diffusion and cooling/solidification process Always reaches eutectic point EMA 5001 Physical Properties of Materials Zhe Cheng (2016) 14 Alloy Solidification k XS XL XL X0/k XE XB 6 Solidification of Single Phase Alloys (6) T Continue from p.6 Evolution of composition profile XB k T1 < T=T2 < T3 T1 T2 T3 TE Liquid X0 kX0 XS kX0 X0 kX0 X0 Solid k XL x Solid XB XS XL T = T3 XB Liquid XL XS x EMA 5001 Physical Properties of Materials X0 Xmax X0/k XE XB Final T TE Solid XE X0 kX0 Zhe Cheng (2016) x 14 Alloy Solidification 7 Constitutional Supercooling Solidification of an alloy with solid grows into superheated liquid Example: Solidification of liquid alloy in a mold w/ wall colder is than liquid “Equilibrium” temperature TEq changes as liquid composition changes near the interface If actual dT/dx is steep as in this region, will form T TC Ti=Tm Solid XB X0 kX0 planar solid/liquid interface as T > TEq T TEq k If actual dT/dx is gradual as in this region, will form cellular or dendrite structure as T < TEq T1 - or constitutional supercooling T3 TE Liquid X0 k XL kX0 XS X0 Xmax X0/k XE XB x EMA 5001 Physical Properties of Materials XS XL 8 Zhe Cheng (2016) 14 Alloy Solidification
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