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 129
... computed . Since the matrix T is independent of concentration for the SS2 and Chebychev bases , the concentration - independence of the Chebychev CEC's implies concentration independence of those in SS2 . II . Cluster Expansion ...
... computed . Since the matrix T is independent of concentration for the SS2 and Chebychev bases , the concentration - independence of the Chebychev CEC's implies concentration independence of those in SS2 . II . Cluster Expansion ...
Page 130
... computed for pure bcc Cr , bcc V , and bcc Ti using the Linear - Muffin - Tin - Orbital ( LMTO ) method in the atomic - sphere - approximation ( ASA ) . The volume of the equiatomic alloy given by Vegard's Law using these volumes was ...
... computed for pure bcc Cr , bcc V , and bcc Ti using the Linear - Muffin - Tin - Orbital ( LMTO ) method in the atomic - sphere - approximation ( ASA ) . The volume of the equiatomic alloy given by Vegard's Law using these volumes was ...
Page 200
... computed phase diagram should not be taken as an accurate assessment of the real real thermodynamic equilibrium in this system , but just as an illustration of the effects of vibrations on computed phase diagrams . We have further ...
... computed phase diagram should not be taken as an accurate assessment of the real real thermodynamic equilibrium in this system , but just as an illustration of the effects of vibrations on computed phase diagrams . We have further ...
Contents
CONSEQUENCES OF OSCILLATORY POTENTIALS AND ANGULAR | 13 |
FIRSTPRINCIPLES TIGHTBINDING TOTAL ENERGY | 25 |
Contributed Papers | 33 |
Copyright | |
30 other sections not shown
Common terms and phrases
10Ti alloy Acta Metall Al-Li 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 measured 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 |