Treatise on Materials Science and TechnologyHerbert Herman |
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Page 92
... normal forces ( 2.14 ) is small needs justification ( van der Merwe , 1963a ) . Recall that these are the forces which come about as a consequence of the fact that the tangential forces ... Normal Forces Appendix B Normal Forces Model.
... normal forces ( 2.14 ) is small needs justification ( van der Merwe , 1963a ) . Recall that these are the forces which come about as a consequence of the fact that the tangential forces ... Normal Forces Appendix B Normal Forces Model.
Page 236
... normal areas cannot be discontinuous . Changes in the density n , of Cooper pairs cannot occur within less than the ... normal and superconducting area . Let AGso be the difference between the specific free energy of a metal in the ...
... normal areas cannot be discontinuous . Changes in the density n , of Cooper pairs cannot occur within less than the ... normal and superconducting area . Let AGso be the difference between the specific free energy of a metal in the ...
Page 238
... normal state at H. with the possibility of super- cooling the normal state ( nucleation problems because of the positive surface energy ) . Figure 4a shows a typical magnetization curve . ( a ) ( b ) -4πMA ( c ) Hc -4πMA TYPE I TYPE II ...
... normal state at H. with the possibility of super- cooling the normal state ( nucleation problems because of the positive surface energy ) . Figure 4a shows a typical magnetization curve . ( a ) ( b ) -4πMA ( c ) Hc -4πMA TYPE I TYPE II ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
11 other sections not shown
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angle anisotropy Appl approximation assumed atoms average axis c-sites calculated cations coherent concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing interaction interface ions lattice length Lett limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reference region relation resolution respectively sample scattering cross section shown shows single solid solution space strain stress structure substrate superconducting surface Table temperature tetrahedral theory thermal thickness transition unit values vector X-ray