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 127
... given function of configuration . Given such a set of ECI's , it is then possible to perform calculations of the ground states of order and of the finite - temperature properties of a given alloy system . Finite - temperature phase ...
... given function of configuration . Given such a set of ECI's , it is then possible to perform calculations of the ground states of order and of the finite - temperature properties of a given alloy system . Finite - temperature phase ...
Page 131
... given by the vertices of some multidimensional polytope in a space spanned by a set of cluster functions ( e.g. Eqn . 2 ) . For a given range of interatomic interactions which is bounded by some maximal interaction cluster ( s ) ( IC's ) ...
... given by the vertices of some multidimensional polytope in a space spanned by a set of cluster functions ( e.g. Eqn . 2 ) . For a given range of interatomic interactions which is bounded by some maximal interaction cluster ( s ) ( IC's ) ...
Page 138
... given temperature T and for a given chemical potential μ . A sample of the crystal that contains a large but finite number of atoms with a specific lattice structure is created within the computer . A typical number of atoms for the fcc ...
... given temperature T and for a given chemical potential μ . A sample of the crystal that contains a large but finite number of atoms with a specific lattice structure is created within the computer . A typical number of atoms for the fcc ...
Contents
CONSEQUENCES OF OSCILLATORY POTENTIALS AND ANGULAR | 13 |
FIRSTPRINCIPLES TIGHTBINDING TOTAL ENERGY | 25 |
Contributed Papers | 33 |
Copyright | |
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Common terms and phrases
addition aging agreement alloys approach approximation atoms average band behavior binary bonding boundary calculations cell chemical cluster compared composition compounds computed concentration configuration consistent contribution correlation crystal defects density dependence described determined diffraction discussed dislocation disordered displacement distance effect elastic electronic electronic structure elements energy expansion experiment experimental FeAl Figure formation function given grain boundaries important included increase indicates interactions intermetallic lattice magnetic Materials matrix measured mechanical Metals method neighbor NiAl observed obtained occupation ordered orientation pair parameters phase diagram Phys Physics plane potential predicted present properties range References relative respectively samples scattering Science shown simulations solid solution stability Stocks strain strength stress structure surface Table techniques temperature ternary theory total energy transition vacancy vibrational volume x-ray yield
References to this book
Encyclopedia of Applied Physics, Volume 18 George L. Trigg,Eduardo S. Vera,Walter Greulich No preview available - 1997 |