## Introduction to Solid State Physicsproblems after each chapter |

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Page 158

If we are far enough away from the individual dipoles of a uniformly polarized

specimen , we may , according to an elementary transformation occurring in

electrostatic theory , calculate the field of the specimen as equal to the field of a

If we are far enough away from the individual dipoles of a uniformly polarized

specimen , we may , according to an elementary transformation occurring in

electrostatic theory , calculate the field of the specimen as equal to the field of a

**surface**...Page 267

strike unit area of the

factor representing quantum reflection effects which we neglect . Then 2e po poro

dp , dp , dE ( 10 . 110 ) h3 J - J - Jų + Er e ( E - Ep ) / kt + 1 = 287 5 . . log ( 1 + 84 ...

strike unit area of the

**surface**will be the emission current density j . apart from afactor representing quantum reflection effects which we neglect . Then 2e po poro

dp , dp , dE ( 10 . 110 ) h3 J - J - Jų + Er e ( E - Ep ) / kt + 1 = 287 5 . . log ( 1 + 84 ...

Page 544

We note that the presence of a screw dislocation transforms successive atom

planes into the

Compound and ring dislocations may be formed from segments of edge and

screw ...

We note that the presence of a screw dislocation transforms successive atom

planes into the

**surface**of a helix , accounting for the name of the dislocation .Compound and ring dislocations may be formed from segments of edge and

screw ...

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### Contents

DIFFRACTION OF XRAYS BY CRYSTALS | 44 |

CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |

ELASTIC CONSTANTS OF CRYSTALS | 85 |

Copyright | |

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### Common terms and phrases

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 neighbor 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