Introduction to Solid State Physicsproblems after each chapter |
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Page 95
Thus the relation ( 4.29 ) is the condition that the crystal should be elastically isotropic ; that is , that waves should propagate in all directions with equal velocities . However , the longitudinal wave velocity is not necessarily ...
Thus the relation ( 4.29 ) is the condition that the crystal should be elastically isotropic ; that is , that waves should propagate in all directions with equal velocities . However , the longitudinal wave velocity is not necessarily ...
Page 180
In this case the polarization charge density on the upper and lower faces of the cube is uniform and equal to + P , while the other faces do not carry any charge . Show that , for this cavity , E2 41P / 3 , just as for the spherical ...
In this case the polarization charge density on the upper and lower faces of the cube is uniform and equal to + P , while the other faces do not carry any charge . Show that , for this cavity , E2 41P / 3 , just as for the spherical ...
Page 553
Motion of the boundary took place by cooperative motion of the dislocations in the array , each dislocation moving an equal distance in its own slip plane . Opposite top and bottom intersections at the boundary with the surface moved ...
Motion of the boundary took place by cooperative motion of the dislocations in the array , each dislocation moving an equal distance in its own slip plane . Opposite top and bottom intersections at the boundary with the surface moved ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone