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Published byNancy Kelly Modified over 6 years ago
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Evolution of Solutions Thermodynamics of mechanical alloying
& mechanical de-alloying
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oxide dispersion strengthened metals
Mechanically alloyed oxide dispersion strengthened metals
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Fe-20Cr-5Al-0.5Ti-0.3 yttria wt%
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Helical grains
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Atom probe image of MA957
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MA956
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MA956
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Binary solution
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Entropy P P / 2
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For a random mixture, number of configurations given by:
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Boltzmann
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Classical theory for entropy of mixing
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Solution-like behaviour when particles about 1000 atoms in size
Free energy of mixing due to configurational entropy alone
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Enthalpy
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Sv Surface per unit volume Solution formation impossible!
Particle size
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coherent coherent incoherent
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Single barrier to solution formation when components attract
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Double barrier to solution formation when components immiscible
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Barrier to solution formation
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Barrier to solution formation, especially in rich solutions
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m o B m o A Paradox at concentration extremities vanishes in the discrete model of concentration Gibbs free energy per mole A B Concentration x of B
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Molar Gibbs free energy
ferrite cementite Molar Gibbs free energy m o Fe Fe x x x a q Concentration of carbon
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Atom probe image of Scifer,
5.5 GPa steel wire
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Scifer, 5.5 GPa with ductility!
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Mechanical de-alloying a a¢ m Molar Gibbs free energy of ferrite Fe x
Concentration of carbon
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Exceptional alloys of iron
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Mechanical tempering
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Mechanical tempering
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Mechanical tempering
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