Introduction to Solid State Physicsproblems after each chapter |
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Page 36
+ + + + + O + + + ( a ) ( b ) • First - layer atoms o Second - layer atoms ++ Third -
layer atoms o Fig . 1.26 . Modes of superposition of close - packed layers of
spheres in ( a ) cubic close - packing and ( b ) hexagonal close - packing .
DIAMOND ...
+ + + + + O + + + ( a ) ( b ) • First - layer atoms o Second - layer atoms ++ Third -
layer atoms o Fig . 1.26 . Modes of superposition of close - packed layers of
spheres in ( a ) cubic close - packing and ( b ) hexagonal close - packing .
DIAMOND ...
Page 65
IONIC CRYSTALS In ionic crystals electrons are transferred from atoms of one
type to atoms of a second type , so that the crystal is made up of positive and
negative ions . The ions arrange themselves so the Coulomb attraction between
ions ...
IONIC CRYSTALS In ionic crystals electrons are transferred from atoms of one
type to atoms of a second type , so that the crystal is made up of positive and
negative ions . The ions arrange themselves so the Coulomb attraction between
ions ...
Page 560
The strength of dilute solid solutions appears to result from the pinning of
dislocations by solute atoms . Cottrell has pointed out that the solubility of a
foreign atom will be greater in the neighborhood of a dislocation than elsewhere
in a crystal .
The strength of dilute solid solutions appears to result from the pinning of
dislocations by solute atoms . Cottrell has pointed out that the solubility of a
foreign atom will be greater in the neighborhood of a dislocation than elsewhere
in a crystal .
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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