Evolution of Solutions Thermodynamics of Mechanical Alloying - PowerPoint PPT Presentation

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Evolution of Solutions Thermodynamics of Mechanical Alloying

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Title: Evolution of Solutions Thermodynamics of Mechanical Alloying


1
Evolution of SolutionsThermodynamics of
Mechanical Alloying
A. Badmos and H. K. D. H. Bhadeshia, Metall.
Mater. Trans. A, 18A (1997) 2189. H. K. D. H.
Bhadeshia, Proceedings of the Royal
Microscopical Society, 35 (2000) 95. Materials
Science and Technology, 16 (2000) 1404. H. K. D.
H. Bhadeshia H. Harada, Applied Surface
Science, 67 (1993) 328.
2
Mechanically Alloyed Oxide Dispersion
Strengthened Metals
3
Normal Grain Size
Sub Micron Grain Size
Grain junctions powerful pinning points for small
grains, which are no longer topologically
independent
4
Fe-20Cr-5Al-0.5Ti-0.3 yttria wt 90 reduction
Capdevila Bhadeshia, 2000
5
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6
Helical grains
Capdevila Bhadeshia, 2000
7
Capdevila Bhadeshia, 2000
8
Atom probe image of MA957
9
MA956
Chou Bhadeshia, 1994
10
MA956
Chou Bhadeshia, 1994
11
Mechanical Mixture
free energy of
mechanical
o
m
mixture
B
G
o
m
Gibbs free energy per mole
A
x
1-x
A
B
Concentration x of B
12
free energy of
mechanical
o
m
mixture
B
G
Gibbs free energy per mole
o
m
A
?G
M
Gx
free energy
of solution
A
B
x
Composition
13
Entropy
P
P / 2
14


15
For a random mixture, number of configurations
given by
16
Boltzmann
17
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18
Classical theory for entropy of mixing
19
Solution-like behaviour when particles about 1000
atoms in size
Free energy of mixing due to configurational
entropy alone
20
Enthalpy
21
Surface per unit volume
Sv
Solution formation impossible!
Particle size
22
coherent
coherent
incoherent
23
Single barrier to solution formation when
components attract
Badmos and Bhadeshia, 1997
24
Double barrier to solution formation when
components immiscible
Badmos and Bhadeshia, 1997
25
Barrier to solution formation
Badmos and Bhadeshia, 1997
26
Barrier to solution formation, especially in rich
solutions
Badmos and Bhadeshia, 1997
27
o
m
B
o
m
A
Gibbs free energy per mole
A
B
Paradox at concentration extremities vanishes in
the discrete model of concentration
Concentration x of B
28
ferrite
cementite
o
Molar Gibbs free energy
m
Fe
Fe
x
x
x
q
a
Concentration of carbon
29
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30
Atom probe image of Scifer, 5.5 GPa steel wire
Bhadeshia and Harada, 1993
31
Scifer, 5.5 GPa with ductility!
Kobe Steel
32
Mechanical tempering
o
m
Fe
Molar Gibbs free energy of ferrite
Fe
x
x
x
a
a
Concentration of carbon
33
Amorphous phase formation during mechanical
alloying of Cu and Cd powders
.contribution from Cu/d interfaces, and
accompanying increase in free energy, provide
additional driving force for amorphisation.
Zhang Massalski Metall. Mater. Trans. 29A
(1998) 2425
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