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 79
... strain . This strain can be chosen so that the energy is an even func- tion of the strain , and at the same time , in the case of cubic phases , preserves the volume of the unit cell [ 6 ] . The following ( monoclinic ) strain tensor ...
... strain . This strain can be chosen so that the energy is an even func- tion of the strain , and at the same time , in the case of cubic phases , preserves the volume of the unit cell [ 6 ] . The following ( monoclinic ) strain tensor ...
Page 162
... strain . First , there was a tendency of the particles to develop pronounced facets along < 100 > directions . This type of transition at relatively small particle sizes can be understood in terms of the competition between the elastic ...
... strain . First , there was a tendency of the particles to develop pronounced facets along < 100 > directions . This type of transition at relatively small particle sizes can be understood in terms of the competition between the elastic ...
Page 216
... strain . Existing first - principle models of alloy structure neglect local strain or treat strain in the low - solute - concentration limit where order is relatively unimportant . Alternatively , models can treat fully ordered alloys ...
... strain . Existing first - principle models of alloy structure neglect local strain or treat strain in the low - solute - concentration limit where order is relatively unimportant . Alternatively , models can treat fully ordered alloys ...
Contents
CONSEQUENCES OF OSCILLATORY POTENTIALS AND ANGULAR | 13 |
FIRSTPRINCIPLES TIGHTBINDING TOTAL ENERGY | 25 |
Contributed Papers | 33 |
Copyright | |
31 other sections not shown
Common terms and phrases
40Ti 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 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 |