## Introduction to Solid State Physicsproblems after each chapter |

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Page 273

2 ( a ) we have indicated the general nature of the variation of the electrostatic

monatomic linear lattice . We expect the ion cores to bear a positive charge , as V

...

2 ( a ) we have indicated the general nature of the variation of the electrostatic

**potential**energy of a conduction electron in the field of the positive ion cores of amonatomic linear lattice . We expect the ion cores to bear a positive charge , as V

...

Page 571

The problem is to calculate the electrostatic

the presence of all the other ions in the crystal . ... We compute the total

A . 1 ) y = $ 1 + 42 at an ion as the sum of two distinct but related

The problem is to calculate the electrostatic

**potential**experienced by one ion inthe presence of all the other ions in the crystal . ... We compute the total

**potential**(A . 1 ) y = $ 1 + 42 at an ion as the sum of two distinct but related

**potentials**.Page 574

The of their Gaussian distributions overlapping the reference point .

due to three contributions from each ion point : 1 1 in por ) quri tr s Iri rido where

the terms are from the point charge , from the part of the Gaussian distribution

lying ...

The of their Gaussian distributions overlapping the reference point .

**potential**isdue to three contributions from each ion point : 1 1 in por ) quri tr s Iri rido where

the terms are from the point charge , from the part of the Gaussian distribution

lying ...

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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 mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present 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