Treatise on Materials Science and TechnologyHerbert Herman |
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Page 20
... consider these briefly . On using operations of the kind ૦૬ дп = αξ δρ dp дп • = - ax sin 0 αξ dp it easily follows that Eqs . ( 3.17 ) transform into . 0 = πW , sin 2π1⁄2 - 142 { a , 2 ( 20,2 sin2 0 x - d2 + a , 2 cos20 dp2 Whe com ...
... consider these briefly . On using operations of the kind ૦૬ дп = αξ δρ dp дп • = - ax sin 0 αξ dp it easily follows that Eqs . ( 3.17 ) transform into . 0 = πW , sin 2π1⁄2 - 142 { a , 2 ( 20,2 sin2 0 x - d2 + a , 2 cos20 dp2 Whe com ...
Page 22
... consider a specific case , say 1 > 0 with б , and bx > ax · x + b . Single Dislocation . For a simple introduction to the concepts involved it is useful to consider the limiting case E1x = 0 ( kx = 1 ) ( 3.35 ) which corresponds to the ...
... consider a specific case , say 1 > 0 with б , and bx > ax · x + b . Single Dislocation . For a simple introduction to the concepts involved it is useful to consider the limiting case E1x = 0 ( kx = 1 ) ( 3.35 ) which corresponds to the ...
Page 231
... Consider Fig . 1 . Just above its superconducting transition temperature , the Nb - Ti alloy has an electrical resistivity four orders of magnitude greater than that of high purity copper . Just below its transition temperature , the ...
... Consider Fig . 1 . Just above its superconducting transition temperature , the Nb - Ti alloy has an electrical resistivity four orders of magnitude greater than that of high purity copper . Just below its transition temperature , the ...
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