Introduction to Solid State Physicsproblems after each chapter |
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Page 51
As an example we show that a fce lattice has as its reciprocal a bec lattice . In the
direct foc lattice the distance between lattice planes in each cube edge direction
is a / 2 , where a is the lattice constant ; thus there are points in the reciprocal ...
As an example we show that a fce lattice has as its reciprocal a bec lattice . In the
direct foc lattice the distance between lattice planes in each cube edge direction
is a / 2 , where a is the lattice constant ; thus there are points in the reciprocal ...
Page 173
In molecular solids the ability of a molecule to rotate depends very much on its
shape and on the strength of its interactions with the environment . The closer the
approach to sphericity and the lower the dipole moment , the more easily the ...
In molecular solids the ability of a molecule to rotate depends very much on its
shape and on the strength of its interactions with the environment . The closer the
approach to sphericity and the lower the dipole moment , the more easily the ...
Page 558
The elastic energy of a dislocation loop of radius r is 2nr times its energy per unit
length , or arGb ?. If the loop is formed in the presence of a shear stress o , the
energy of the crystal will decrease by the product of ob and the area of the loop ...
The elastic energy of a dislocation loop of radius r is 2nr times its energy per unit
length , or arGb ?. If the loop is formed in the presence of a shear stress o , the
energy of the crystal will decrease by the product of ob and the area of the loop ...
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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