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Fundamentals of Solidification Lecture 4: Nucleation and growth
Outline ,[object Object],[object Object],[object Object],[object Object],[object Object]
Introduction ,[object Object],[object Object],[object Object],[object Object],[object Object]
Temperature vs. time in glass solidification and phase transition solidification
Viscosity vs. temperature in glass solidification and phase transition solidification (a) Glass solidification  (b) Phase-transition solidification
Density vs. temperature in glass solidification and phase transition solidification
Heat capacity of Fe
Introduction ,[object Object],[object Object],[object Object],[object Object],[object Object]
Homogeneous nucleation r r
Homogeneous nucleation ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Local free energy change 1. Liquid to solid  2. Interface
Local free energy change Spherical nucleus:
Single nucleus
Critical radius
(G L -G S ) vs. supercooling Free energy density vs. temperature  liquid solid temperature Free energy density
Parameters For FCC Copper, r*  1 nm, which contains 310 Cu atoms in each nucleus.
System free energy ,[object Object],[object Object],[object Object]
Number of nuclei ,[object Object]
when Number of nuclei Boltzmann formula:   Critical nuclei:
Heterogeneous nucleation ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Heterogeneous nucleation Liquid  Inclusion  Nucleus    IL  NL  IN R r h a 
Force equilibrium where   IL ,   IN  and   NL  are the interface energies of inclusion-liquid, inclusion-nucleus and nucleus-liquid, respectively.    is the nucleus-inclusion wetting angle. The nucleus is a spherical cap of  radius  r.  Heterogeneous nucleation
Free energy change
Free energy change Using
Thermodynamic barriers Heterogeneous nucleation barrier  Homogeneous  nucleation barrier
Thermodynamic barrier vs. wetting angle
 
Number of nuclei with critical radius  where  n s  is the total number of atom around the incubating agents’ surface in liquid.
Inoculating agents ,[object Object],[object Object],[object Object],[object Object],[object Object]
Casting refinement  ,[object Object],[object Object],[object Object],[object Object],[object Object]
Growth and microstructure T. F. Brower and M.C. Flemings, Trans. AIME, 239, 1620 (1967)
Growth and microstructure H.B. Dong and P.D. Lee, Acta Mater. 53 (2005) 659
Outer chilled zones
Outer chilled zones
Outer chilled zones
Outer chilled zones Pure metals: Formation of shell because temperature gradient is the key factor in grain growth.
Outer chilled zones re-melted? Pouring temperature survived?
Microstructure of ingot ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Intermediate columnar zone Columnar grains grows The grain is overtaken by neighbors.
Intermediate columnar zone Growth and overtaken
Intermediate columnar zone Columnar growth blocked
Central equiaxed zone  ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Structure and properties
Summary ,[object Object],[object Object],[object Object],[object Object]

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