## Introduction to Solid State Physics |

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Page 177

The essential difference between

for transformer cores lies in the coercive force , which may range from the value

of 600 oersteds in a loudspeaker magnet ( Alnico V ) and 20 , 000 in a special

high ...

The essential difference between

**material**for permanent magnets and**material**for transformer cores lies in the coercive force , which may range from the value

of 600 oersteds in a loudspeaker magnet ( Alnico V ) and 20 , 000 in a special

high ...

Page 219

become normal ; the effective shape of the superconducting

become something like a prolate spheroid , thereby reducing the field in the

interior . The

regions ...

become normal ; the effective shape of the superconducting

**material**will thenbecome something like a prolate spheroid , thereby reducing the field in the

interior . The

**material**at the boundary between normal and superconductingregions ...

Page 301

Make a cut along any simple surface bounded by the line . Displace the

on one side of this surface by d relative to the other side ; d is a fixed vector called

the Burgers vector . In regions where d is not parallel to the surface this relative ...

Make a cut along any simple surface bounded by the line . Displace the

**material**on one side of this surface by d relative to the other side ; d is a fixed vector called

the Burgers vector . In regions where d is not parallel to the surface this relative ...

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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