Alloy Modeling & Design: Proceedings of a Symposium Sponsored by the TMS Structural Materials Division (SMD), the Committee on Alloy Phases (CAP), and the Electronic, Magnetic and Photonic Materials Division (EMPMD), the Oak Ridge National Laboratory and the Lawrence Livermore National Laboratory, Held During Materials Week '93, Pittsburgh, Pennsylvania, October 18-20, 1993G. M. Stocks, Patrice E. A. Turchi This work brings together contributions from researchers in a variety of fields that have a common interest in applying the most recent developments in basic research to the design of new alloys. The papers are from Materials Week '93 held in Pittsburgh, Pennsylvania, October 17-21, 1993. |
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Page 4
... unit cells . In addition to the complex alloy phases often seen in real ... cell and ẞ ( Al3 Mg2 ) with a complex face centered cubic ( fcc ) structure ... unit cell systems and for transition metals , oxides , and carbides . However , as ...
... unit cells . In addition to the complex alloy phases often seen in real ... cell and ẞ ( Al3 Mg2 ) with a complex face centered cubic ( fcc ) structure ... unit cell systems and for transition metals , oxides , and carbides . However , as ...
Page 29
... primitive unit cell of the system , and a wavevector q which is commensurate with the supercell , then , if the atom at location R in the supercell is displaced by an amount SR u cos q⋅ R , the total energy changes by an amount △ E α ...
... primitive unit cell of the system , and a wavevector q which is commensurate with the supercell , then , if the atom at location R in the supercell is displaced by an amount SR u cos q⋅ R , the total energy changes by an amount △ E α ...
Page 110
... unit cells smaller than 32. The remaining 940 vertices are either inconstructable or have a unit cell with more than 32 atoms . The two - dimensional projections of the 31 structures are shown in fig . 1 . The For some of the structures ...
... unit cells smaller than 32. The remaining 940 vertices are either inconstructable or have a unit cell with more than 32 atoms . The two - dimensional projections of the 31 structures are shown in fig . 1 . The For some of the structures ...
Contents
CONSEQUENCES OF OSCILLATORY POTENTIALS AND ANGULAR | 13 |
FIRSTPRINCIPLES TIGHTBINDING TOTAL ENERGY | 25 |
Contributed Papers | 33 |
Copyright | |
29 other sections not shown
Common terms and phrases
10Ti alloy Acta Metall Al-Li Al3Ti Alloy Modeling Alloy Phase alloys annealing APB energy approximation atom probe behavior binary alloys cluster expansion composition computed configuration density Design Edited dislocation displacement ductility Edited by G.M. effect elastic constants electronic structure entropy equivolume expansion experimental FeAl Fermi energy Fermi surface Figure first-principles formation energy free energy friction stress G.M. Stocks glide plane grain boundaries Grand Potential Hamiltonian increase intermetallic compounds Ising model lattice constants lattice parameter Lett magnetic Materials Science Materials Society matrix Metals & Materials method Modeling and Design nearest neighbor Ni3Al NiAl obtained ordered P.E.A. Turchi phase diagram phase stability phonon Phys plane point defects potential predicted samples screw shown in Fig simulations solid solution Stocks and P.E.A. stoichiometry sublattice techniques ternary theory thermal tight-binding total energy transition metal trialuminides Turchi The Minerals unit cell vibrational x-ray
References to this book
Encyclopedia of Applied Physics, Volume 18 George L. Trigg,Eduardo S. Vera,Walter Greulich No preview available - 1997 |