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B. B. Rath Symposium Thermodynamics of Interfaces in Mechanically Alloyed Metals
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Mechanically Alloyed Oxide Dispersion Strengthened Metals
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Atom probe image of MA957
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MA956 Chou & Bhadeshia, 1994
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MA956 Chou & Bhadeshia, 1994
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o o A B A B 1-x Gibbs free energy per mole Concentration x of B free energy of mechanical mixture G* x Mechanical Mixture
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o o A B A B x Gibbs free energy per mole Composition G{x} free energy of mechanical mixture ∆G M free energy of solution G*
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Entropy P P / 2
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+=
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For a random mixture, number of configurations given by:
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Boltzmann
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Badmos and Bhadeshia, 1997
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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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Surface per unit volume SvSv Particle size Solution formation impossible!
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coherent incoherent
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Single barrier to solution formation when components attract Badmos and Bhadeshia, 1997
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Double barrier to solution formation when components immiscible Badmos and Bhadeshia, 1997
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o o A B A B Gibbs free energy per mole Concentration x of B Paradox at concentration extremities vanishes in the discrete model of concentration
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Amorphous phase formation during mechanical alloying of Cu and Cd powders Zhang & Massalski Metall. & Mater. Trans. 29A (1998) 2425 ….contribution from Cu/ interfaces, and accompanying increase in free energy, provide additional driving force for amorphisation….
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Capdevila & Bhadeshia, 2000 MA957, 1330 - 30 °C
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Sub Micron Grain Size Normal Grain Size Grain junctions powerful pinning points for small grains, which are no longer topologically independent
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Evolution of Solutions Thermodynamics 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.
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