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. |
From inside the book
Results 1-3 of 80
Page 123
... shown . In calculating the phase diagram shown in Fig . 2 ( a ) , the elastic contributions to the alloy free energy due to structural - relaxations , as well as the vibrational enthalpy and entropy were neglected . The Cd3Mg and CdMg ...
... shown . In calculating the phase diagram shown in Fig . 2 ( a ) , the elastic contributions to the alloy free energy due to structural - relaxations , as well as the vibrational enthalpy and entropy were neglected . The Cd3Mg and CdMg ...
Page 189
... shown in Figure 6 . Two { 111 } planes are shown . The glide plane is shown as the atoms connected by the wire mesh , with the atoms in the plane above the glide plane shown without a mesh , but with the near neighbor bonds connecting ...
... shown in Figure 6 . Two { 111 } planes are shown . The glide plane is shown as the atoms connected by the wire mesh , with the atoms in the plane above the glide plane shown without a mesh , but with the near neighbor bonds connecting ...
Page 278
... shown in Fig . 2. It is shown that in alloys B and C the morphology of the second phase NiBe is ascicular , while a finer mixture of two phases is attained in alloys G and H. In Figure 3 is shown the estimated liquidus surface from the ...
... shown in Fig . 2. It is shown that in alloys B and C the morphology of the second phase NiBe is ascicular , while a finer mixture of two phases is attained in alloys G and H. In Figure 3 is shown the estimated liquidus surface from the ...
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 |