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. |
From inside the book
Results 1-3 of 58
Page 67
... crystal the I - V pair occupys . However , the sequence of the binding energies of the I - V pairs with different kinds solutes of I on a specific pair site of the crystal cell well corresponds to that of the measured self ...
... crystal the I - V pair occupys . However , the sequence of the binding energies of the I - V pairs with different kinds solutes of I on a specific pair site of the crystal cell well corresponds to that of the measured self ...
Page 68
... crystal of NiŠ·Al , respectively , and 6E1_v is that due to simaltaneous introduction of I and V into the crystal as a pair of I and V. Each of these energy changes essentially consists of two terms of the band structure and repulsive ...
... crystal of NiŠ·Al , respectively , and 6E1_v is that due to simaltaneous introduction of I and V into the crystal as a pair of I and V. Each of these energy changes essentially consists of two terms of the band structure and repulsive ...
Page 167
... crystal energy surfaces for a limited type of crystal structure changes of pure elemental , as well as intermetallic phases . These crystal structure changes consist of volume expansion ( contraction ) , and fixed volume lattice ...
... crystal energy surfaces for a limited type of crystal structure changes of pure elemental , as well as intermetallic phases . These crystal structure changes consist of volume expansion ( contraction ) , and fixed volume lattice ...
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 |