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 108
... Alloy Phases (CAP), and the Electronic, Magnetic and Photonic Materials Division (EMPMD), the Oak Ridge National Laboratory and the Lawrence Livermore Nat G. M. Stocks, Patrice E. A. Turchi. 1. Introduction Binary alloy phase diagrams ...
... Alloy Phases (CAP), and the Electronic, Magnetic and Photonic Materials Division (EMPMD), the Oak Ridge National Laboratory and the Lawrence Livermore Nat G. M. Stocks, Patrice E. A. Turchi. 1. Introduction Binary alloy phase diagrams ...
Page 128
... binary alloys are now made with regularity ( see for example Ref's . [ 1-3 ] ) , and it has been shown that the problem of configurational disorder in binary substitutional alloys can be treated quite effectively [ 4,5 ] . Ternary ...
... binary alloys are now made with regularity ( see for example Ref's . [ 1-3 ] ) , and it has been shown that the problem of configurational disorder in binary substitutional alloys can be treated quite effectively [ 4,5 ] . Ternary ...
Page 264
... binary alloys is sensitive to the concentration of excess Fe distributed on the Al sublattice as shown in Fig . 6. The excess Fe plus an additional amount equal to the Al on the Fe sublattice resides on the Al sublattice and is plotted ...
... binary alloys is sensitive to the concentration of excess Fe distributed on the Al sublattice as shown in Fig . 6. The excess Fe plus an additional amount equal to the Al on the Fe sublattice resides on the Al sublattice and is plotted ...
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 |