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 14
Page 239
... quenching from different temperatures and those calculated from the vacancy concentrations shown in Fig . 2. Fast cooling ( i.e. , cooling in vacuum at room temperature ) from 1273 K results in much higher strengths , in agreement with ...
... quenching from different temperatures and those calculated from the vacancy concentrations shown in Fig . 2. Fast cooling ( i.e. , cooling in vacuum at room temperature ) from 1273 K results in much higher strengths , in agreement with ...
Page 307
... Quenched from the homogenisation temperature , this alloy contains only ẞ phase ; no martensite of any form was found . After annealing at 600 ° C for 48h , a new LPS phase with a 6R stacking variation forms from the ẞ phase , as can be ...
... Quenched from the homogenisation temperature , this alloy contains only ẞ phase ; no martensite of any form was found . After annealing at 600 ° C for 48h , a new LPS phase with a 6R stacking variation forms from the ẞ phase , as can be ...
Page 308
... quenching , but during isothermal annealing at intermediate temperatures ; the second factor is that atomic ordering has occurred in the basal plane of the LPS structures . These transformations share the displacive feature with ...
... quenching , but during isothermal annealing at intermediate temperatures ; the second factor is that atomic ordering has occurred in the basal plane of the LPS structures . These transformations share the displacive feature with ...
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 |