Introduction to Solid State Physicsproblems after each chapter |
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Page 18
Rotation axis : X Rotation - inversion axis : X Rotation axis with mirror plane
normal to it : X / m or - Rotation axis with diad axis ( axes ) normal to it : X2
Rotation axis with mirror plane ( planes ) parallel to it : Xm Rotation - inversion
axis with ...
Rotation axis : X Rotation - inversion axis : X Rotation axis with mirror plane
normal to it : X / m or - Rotation axis with diad axis ( axes ) normal to it : X2
Rotation axis with mirror plane ( planes ) parallel to it : Xm Rotation - inversion
axis with ...
Page 88
In one of the shears , planes of the material normal to the x axis slide in the y
direction ; in the other shear , planes normal to y slide in the x direction . STRESS
COMPONENTS The force acting on a unit area in the solid is defined as the
stress .
In one of the shears , planes of the material normal to the x axis slide in the y
direction ; in the other shear , planes normal to y slide in the x direction . STRESS
COMPONENTS The force acting on a unit area in the solid is defined as the
stress .
Page 471
48 ) H > - H . When this situation occurs we can avoid having the whole sphere
become normal by having the material around the equator of the sphere become
normal ; the effective shape of the superconducting material will then become ...
48 ) H > - H . When this situation occurs we can avoid having the whole sphere
become normal by having the material around the equator of the sphere become
normal ; the effective shape of the superconducting material will then become ...
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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 neighbor normal observed obtained parallel particles Phys physics plane polarization positive possible potential 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