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Fundamentals of Solidification
Lecture 4: Nucleation and growth
Outline
• Introduction
• Homogeneous nucleation
• Heterogeneous nucleation
• Growth and microstructure
• Summary
Introduction
• There are two types of solidification
– Glass formation
• Physical properties such as viscosity change
smoothly across the solidifying region
– Phase transition
• Some physical properties change abruptly,
such as viscosity, heat capacity
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
• Solidification by phase transition is
modelled as two stage
– Nucleation
• Homogeneous nucleation
• Heterogeneous nucleation
– Growth
Homogeneous nucleation
rr
Homogeneous nucleation
• No preferred nucleation sites
– Spontaneous
– Random
• Those of preferred sites
– Boundary
– Surface
– Inclusion, …
Local free energy change
1. Liquid to solid 2. Interface
Local free energy change
SLLSbeforeafter AGGVGGG
SLSL rGGrG 23 43
4
Spherical nucleus:
Single nucleus
Critical radius
0/ drGd
SL
SL
GGr
2*
2
3
3
16*
SL
SL
GGG
(GL-GS) 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
• Ideal solution: Particle of different sizes
• ni particles with each contains i atoms
• n particles with each contains 1 atom
STGnG ic
ii
ii nn
nn
nn
nnkS lnln
Number of nuclei
• At equilibrium
0/ ic nG
i
i
nn
n
kT
Gln
inn
kT
Gnni exp
kT
Gnni
*exp*
when
Number of nuclei
Boltzmann formula:
Critical nuclei:
Heterogeneous nucleation
• Nucleation site
– Mold walls
– Inclusion
– Interface
– Surface
– Impurity
Liquid
Inclusion
Nucleus IL
NL
IN
R
r
h
a
Heterogeneous nucleation
cosNLINIL
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 cosNLINIL
Thermodynamic barriers
Heterogeneous nucleation barrier
Homogeneous nucleation barrier
Thermodynamic barrier vs. wetting angle
Number of nuclei with critical radius
where ns is the total number of atom around the
incubating agents’ surface in liquid.
Inoculating agents
• Small interface energy
– Similar crystal structure
– Similar lattice distance
– Same physical properties
– Same chemical properties
Casting refinement
• Adding inoculating agents
– Overheat might melt the agents
• Surface refinement
– Coat agents on mold walls
• Pattern induced solidification
Growth and microstructure
T. F. Brower and M.C. Flemings, Trans. AIME, 239, 1620 (1967)
H.B. Dong and P.D. Lee, Acta Mater. 53 (2005) 659
Growth and microstructure
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
• Chilled zone
– Fine equiaxed grains.
– Pure substance: Continuous shell.
– Solution: Particles
– Particles flushed away from wall into the
central
• Re-melted
• Survived – nucleus
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
• Equiaxed grain
– Nucleation:
• Supercooling
• Falling particles
• Dendrite fragments– Elevated pouring
temperature:
• Larger equiaxed grains
• More columnar zone
– Anisotropic properties
• Magnetic materials
• Turbo blade.
• More equiaxed zone
– Isotropic properties
– Less segregation
Structure and properties
Summary
• Casting
• Heat management
• Thermodynamics
• Nucleation and growth