Introduction to Solid State Physicsproblems after each chapter |
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Page 4
We assume that a is the shortest non - vanishing translation in the translation
group . We choose coordinate axes so that a is parallel to the x axis . If now we
rotate a by an angle d , we get a new vector a ' with components ax ' = a cos ; ay =
a ...
We assume that a is the shortest non - vanishing translation in the translation
group . We choose coordinate axes so that a is parallel to the x axis . If now we
rotate a by an angle d , we get a new vector a ' with components ax ' = a cos ; ay =
a ...
Page 50
The vector r * ( hkl ) in the reciprocal lattice is in the same direction but n times as
long as the vector corresponding to the true crystal plane . . That is , the nth point
from the origin in a given row in the reciprocal lattice corresponds to the nth ...
The vector r * ( hkl ) in the reciprocal lattice is in the same direction but n times as
long as the vector corresponding to the true crystal plane . . That is , the nth point
from the origin in a given row in the reciprocal lattice corresponds to the nth ...
Page 544
The material on one side of the cut is displaced relative to that on the other by
vector distance b , which may be arbitrarily oriented relative to the surface .
Forces will be required to effect the displacement . The medium is filled in or cut
away so ...
The material on one side of the cut is displaced relative to that on the other by
vector distance b , which may be arbitrarily oriented relative to the surface .
Forces will be required to effect the displacement . The medium is filled in or cut
away so ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
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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