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 5
... ions move a short distance in each time step , typically 0.01Å , and therefore the eigenvector from the last time step is an excellent input for the current one . ~ We also note that it is not necessary to store the full matrix h , but ...
... ions move a short distance in each time step , typically 0.01Å , and therefore the eigenvector from the last time step is an excellent input for the current one . ~ We also note that it is not necessary to store the full matrix h , but ...
Page 283
... ion microscopy ( APFIM ) and transmission electron microscopy ( TEM ) have been used to investigate the influence of trace metallic impurities on the enormous increase in the yield stress of boron - doped NiAl . Previous atom probe ...
... ion microscopy ( APFIM ) and transmission electron microscopy ( TEM ) have been used to investigate the influence of trace metallic impurities on the enormous increase in the yield stress of boron - doped NiAl . Previous atom probe ...
Page 284
... ion images of the matrix [ 6,7 ] . The precipitates encountered in the field ion microscope ( FIM ) images ranged from < 2 nm to approximately 20 nm in diameter and atom probe measurements of the compositions were consistent with MB2 ...
... ion images of the matrix [ 6,7 ] . The precipitates encountered in the field ion microscope ( FIM ) images ranged from < 2 nm to approximately 20 nm in diameter and atom probe measurements of the compositions were consistent with MB2 ...
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 |