Introduction to Solid State Physicsproblems after each chapter |
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Page 105
... being the increase in length of the bond between atoms n and n + 1 , the
second term being the increase in length of the bond between atoms n and n - 1.
If both bonds increase in length , the two forces on atom n will be oppositely
directed .
... being the increase in length of the bond between atoms n and n + 1 , the
second term being the increase in length of the bond between atoms n and n - 1.
If both bonds increase in length , the two forces on atom n will be oppositely
directed .
Page 414
ency of the g values to decrease as the resonant frequency is increased , 16 and
an explanation of this behavior has been proposed by Kittel and Mitchell . 15
FERROMAGNETIC DOMAINS17 At temperatures well below the Curie point the ...
ency of the g values to decrease as the resonant frequency is increased , 16 and
an explanation of this behavior has been proposed by Kittel and Mitchell . 15
FERROMAGNETIC DOMAINS17 At temperatures well below the Curie point the ...
Page 560
If the alloy is held at a high temperature where some particles grow at the
expense of others , L increases and the strength drops . ... When a dislocation
moves , leaving its solute cloud behind , the energy of the crystal must increase .
If the alloy is held at a high temperature where some particles grow at the
expense of others , L increases and the strength drops . ... When a dislocation
moves , leaving its solute cloud behind , the energy of the crystal must increase .
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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