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 201
... temperatures For most alloy systems , the transition temperatures are larger than the Debye temperatures and the first term in the r.h.s. of ( 5 ) is a good representation of the temperature - dependent vibrational effective ...
... temperatures For most alloy systems , the transition temperatures are larger than the Debye temperatures and the first term in the r.h.s. of ( 5 ) is a good representation of the temperature - dependent vibrational effective ...
Page 256
... temperature . We found that : ( 1 ) . There is no structural transformation in this alloy between room temperature and 700 ° C , ie . , the temary C15 Laves phase based on HFV2 is thermally stable over this entire temperature range ...
... temperature . We found that : ( 1 ) . There is no structural transformation in this alloy between room temperature and 700 ° C , ie . , the temary C15 Laves phase based on HFV2 is thermally stable over this entire temperature range ...
Page 280
... temperature dependence of strength is exhibited , which must come from the nature of the constituent L1 , phase . At temperatures beyond the peak for the mechanical anomaly , rapid decrease in strength with increaing temperature is ...
... temperature dependence of strength is exhibited , which must come from the nature of the constituent L1 , phase . At temperatures beyond the peak for the mechanical anomaly , rapid decrease in strength with increaing temperature is ...
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 |