## 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

.

... 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

changes in domain

Domains oriented unfavorably with respect to the direction of the electric field are

diminished in

**volume**, and favorably oriented domains increase in**volume**. Thechanges 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

... 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 ...### What people are saying - Write a review

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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