Introduction to Solid State Physicsproblems after each chapter |
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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 102
A cubic crystal is subject to tension in the ( 100 ) direction . Find expressions for
Young ' s modulus and Poisson ' s ratio in terms of the elastie compliances or
stiffnesses . 4 . 5 . Show that the velocity of propagation of a shear wave moving ...
A cubic crystal is subject to tension in the ( 100 ) direction . Find expressions for
Young ' s modulus and Poisson ' s ratio in terms of the elastie compliances or
stiffnesses . 4 . 5 . Show that the velocity of propagation of a shear wave moving ...
Page 431
Charles Kittel. MAGNETOSTRICTION It is observed in ferromagnetic single
crystals that the length of the crystal in a given direction relative to the crystal
axes depends in general on the direction of the magnetization relative to the
crystal axes .
Charles Kittel. MAGNETOSTRICTION It is observed in ferromagnetic single
crystals that the length of the crystal in a given direction relative to the crystal
axes depends in general on the direction of the magnetization relative to the
crystal axes .
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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