Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 35
Page 92
... becomes x Pzz ( 0 , x ) = [ 2μ / ( 1-20 ) ] ( W / d ) ( B.1 ) It has only been possible to solve the elastic problem with this extra boundary condition , for the unrealistic parabolic interfacial potential ( 2.4 ) . By inspection of ...
... becomes x Pzz ( 0 , x ) = [ 2μ / ( 1-20 ) ] ( W / d ) ( B.1 ) It has only been possible to solve the elastic problem with this extra boundary condition , for the unrealistic parabolic interfacial potential ( 2.4 ) . By inspection of ...
Page 240
... becomes energetically favorable to produce flux lines . In complete analogy to Eq . ( 10 ) , He1 can be expressed in terms of the free energy per length of a flux line & o ( for H2 = 0 ) and the reduction in magnetic field energy - Ha ...
... becomes energetically favorable to produce flux lines . In complete analogy to Eq . ( 10 ) , He1 can be expressed in terms of the free energy per length of a flux line & o ( for H2 = 0 ) and the reduction in magnetic field energy - Ha ...
Page 255
... becomes smaller , the tunneling results become more dependent on the surface properties . Thus , the tunneling results for the A - 15 compounds are unreliable indicators of bulk properties . Hopfield ( 1972 ) has recently argued that a ...
... becomes smaller , the tunneling results become more dependent on the surface properties . Thus , the tunneling results for the A - 15 compounds are unreliable indicators of bulk properties . Hopfield ( 1972 ) has recently argued that a ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
11 other sections not shown
Common terms and phrases
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