Introduction to Solid State Physicsproblems after each chapter |
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Page 42
Find the space group of the cubic ZnS ( zinc blende ) structure . 1.5 . Show that
the maximum proportion of the available volume which may be filled by hard
spheres arranged in various structures is Simple cubic Body - centered cubic
Face ...
Find the space group of the cubic ZnS ( zinc blende ) structure . 1.5 . Show that
the maximum proportion of the available volume which may be filled by hard
spheres arranged in various structures is Simple cubic Body - centered cubic
Face ...
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 elastic compliances or
stiffnesses . 4.5 . Show that the velocity of propagation of a shear wave moving
along a ...
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 elastic compliances or
stiffnesses . 4.5 . Show that the velocity of propagation of a shear wave moving
along a ...
Page 161
The proof we have given for the vanishing of E3 actually obtains for all cases in
which the environment of the reference point is cubic , as long as the dipoles are
parallel . Thus E3 = 0 for induced polarization on simple cubic , body - centered ...
The proof we have given for the vanishing of E3 actually obtains for all cases in
which the environment of the reference point is cubic , as long as the dipoles are
parallel . Thus E3 = 0 for induced polarization on simple cubic , body - centered ...
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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 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