Introduction to Solid State Physics |
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Page 74
... where the factor 3 arises because elastic waves of given k occur with three
different polarizations which in an isotropic medium reduce to two shear waves
and one longitudinal wave . The internal energy per unit volume is then , from ( 5
.
... where the factor 3 arises because elastic waves of given k occur with three
different polarizations which in an isotropic medium reduce to two shear waves
and one longitudinal wave . The internal energy per unit volume is then , from ( 5
.
Page 129
Domains oriented unfavorably with respect to the direction of the electric field are
diminished in volume , and favorably oriented domains increase in volume . The
changes in domain volume are naturally accompanied by polarization changes ...
Domains oriented unfavorably with respect to the direction of the electric field are
diminished in volume , and favorably oriented domains increase in volume . The
changes in domain volume are naturally accompanied by polarization changes ...
Page 228
... kT « We , and non - degenerate when kT » W , ( classical limit ) . STATISTICS
OF FREE ELECTRON GAS In ( 5 . 12 ) we obtained an expression for the number
of modes of an elastic system , per unit volume , for which the magnitude of the ...
... kT « We , and non - degenerate when kT » W , ( classical limit ) . STATISTICS
OF FREE ELECTRON GAS In ( 5 . 12 ) we obtained an expression for the number
of modes of an elastic system , per unit volume , for which the magnitude of the ...
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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
Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1953 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 396 pages |
| Export Citation | BiBTeX EndNote RefMan |