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 165
... thermal expansions of Ni - rich ( fcc structure ) Ni / Cr alloys ( which serve as the basis for practical superalloy systems ) . This has been done using ab initio interatomic potentials with no experimental input . The coefficient of ...
... thermal expansions of Ni - rich ( fcc structure ) Ni / Cr alloys ( which serve as the basis for practical superalloy systems ) . This has been done using ab initio interatomic potentials with no experimental input . The coefficient of ...
Page 166
... thermal expansion ( CTE ) of high - temperature structural alloys is an important factor in the way they function , for example affecting the interface thermal compatibility with the protecting oxide scale . Theoretical studies of thermal ...
... thermal expansion ( CTE ) of high - temperature structural alloys is an important factor in the way they function , for example affecting the interface thermal compatibility with the protecting oxide scale . Theoretical studies of thermal ...
Page 239
... thermal expansion . Similarly , Ho and Dodd's ( 20 ) plot of the thermal expansion of Fe - 50A1 shows a discontinuity in the slope around 873 K. It is conceivable that this phase transformation has an effect on the point defect ...
... thermal expansion . Similarly , Ho and Dodd's ( 20 ) plot of the thermal expansion of Fe - 50A1 shows a discontinuity in the slope around 873 K. It is conceivable that this phase transformation has an effect on the point defect ...
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
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 |