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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Results 1-3 of 38
Page 110
... correlations and 2 point correlations ) . The configuration polytope in this space was determined ( 6 , 18 ) by formulating constraints on the regular octahedron and tetrahedron clusters . Combined , these two clusters define 71 ...
... correlations and 2 point correlations ) . The configuration polytope in this space was determined ( 6 , 18 ) by formulating constraints on the regular octahedron and tetrahedron clusters . Combined , these two clusters define 71 ...
Page 131
... correlation functions using standard Newton - Raphson techniques , yielding the equilibrium free energy and correlations . The CVM was originally formulated in terms of cluster probabilities ( for both the energy and entropy ) . Since ...
... correlation functions using standard Newton - Raphson techniques , yielding the equilibrium free energy and correlations . The CVM was originally formulated in terms of cluster probabilities ( for both the energy and entropy ) . Since ...
Page 132
... correlation functions is all but necessary to treat correlations beyond the range of NN . The increase in the number of variables needed in CVM calculations in turn has consequences for the computation of the ECI's . The first obvious ...
... correlation functions is all but necessary to treat correlations beyond the range of NN . The increase in the number of variables needed in CVM calculations in turn has consequences for the computation of the ECI's . The first obvious ...
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 |