Introduction to Solid State Physics |
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Page 32
The total binding energy may be attributed almost entirely to the Coulomb energy
, as we shall find that n is of the order of 10 . EVALUATION OF THE MADELUNG
CONSTANT The first calculation of the Coulomb energy constant a was made ...
The total binding energy may be attributed almost entirely to the Coulomb energy
, as we shall find that n is of the order of 10 . EVALUATION OF THE MADELUNG
CONSTANT The first calculation of the Coulomb energy constant a was made ...
Page 36
are known with the sodium chloride structure than with the cesium chloride
structure , but as the differences in binding energy are small we can often only
decide at a given temperature which will be stable for a particular salt by a
consideration ...
are known with the sodium chloride structure than with the cesium chloride
structure , but as the differences in binding energy are small we can often only
decide at a given temperature which will be stable for a particular salt by a
consideration ...
Page 185
Since the exchange energy of a wall is inversely proportional to the thickness (
10 . 37 ) , the wall might spread out until it filled a sizable proportion of the crystal
, were it not for the restraining effect of the anisotropy energy , which acts to limit ...
Since the exchange energy of a wall is inversely proportional to the thickness (
10 . 37 ) , the wall might spread out until it filled a sizable proportion of the crystal
, were it not for the restraining effect of the anisotropy energy , which acts to limit ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero