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Phys. Rev. B 78, 054121 (2008) [10 pages]

Classical potential describes martensitic phase transformations between the α, β, and ω titanium phases

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R. G. Hennig1,2, T. J. Lenosky3, D. R. Trinkle2,4, S. P. Rudin5, and J. W. Wilkins2
1Department of Materials Science and Engineering, Cornell University, Ithaca, New York 14853, USA
2Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA
3C8 Medisensors, San Jose, California 95124, USA
4Department of Materials Science and Engineering, University of Illinois at Urbana Champaign, Urbana, Illinois 61801, USA
5Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA

Received 23 July 2008; published 27 August 2008

A description of the martensitic transformations between the α, β, and ω phases of titanium that includes nucleation and growth requires an accurate classical potential. Optimization of the parameters of a modified embedded atom potential to a database of density-functional calculations yields an accurate and transferable potential as verified by comparison to experimental and density-functional data for phonons, surface and stacking fault energies, and energy barriers for homogeneous martensitic transformations. Molecular-dynamics simulations map out the pressure-temperature phase diagram of titanium. For this potential the martensitic phase transformation between α and β appears at ambient pressure and 1200 K, between α and ω at ambient conditions, between β and ω at 1200 K and pressures above 8 GPa, and the triple point occurs at 8 GPa and 1200 K. Molecular-dynamics explorations of the kinetics of the martensitic α-ω transformation show a fast moving interface with a low interfacial energy of 30 meV/Å2. The potential is applicable to the study of defects and phase transformations of Ti.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.78.054121
DOI:
10.1103/PhysRevB.78.054121
PACS:
64.70.K−, 71.15.Pd, 81.30.Kf, 63.20.−e