Introduction to Solid State Physicsproblems after each chapter |
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Page 84
Suppose that it were possible to permeate the space between ions in an ionic
crystal with a homogeneous fluid of dielectric constant e without affecting the
equation for the repulsive interactions between ions , but reducing the Coulomb ...
Suppose that it were possible to permeate the space between ions in an ionic
crystal with a homogeneous fluid of dielectric constant e without affecting the
equation for the repulsive interactions between ions , but reducing the Coulomb ...
Page 102
Show that in a cubic crystal the effective compliance constant for a shear across
the ( 110 ) plane in the ( 110 ) direction is equal to 2 ( 811 – 812 ) and ... while in
the ( 001 ) direction in the same plane the effective compliance constant is 844 .
Show that in a cubic crystal the effective compliance constant for a shear across
the ( 110 ) plane in the ( 110 ) direction is equal to 2 ( 811 – 812 ) and ... while in
the ( 001 ) direction in the same plane the effective compliance constant is 844 .
Page 169
... and similar liquids , and the temperature dependence of their dielectric
constants . The problem of the dielectric constant of water is that the static
dielectric constant is - CHỊCH o CH C12 Molar polarizability mu CHCig « 4050
avaoca , 0 .
... and similar liquids , and the temperature dependence of their dielectric
constants . The problem of the dielectric constant of water is that the static
dielectric constant is - CHỊCH o CH C12 Molar polarizability mu CHCig « 4050
avaoca , 0 .
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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 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