## Introduction to Solid State Physicsproblems after each chapter |

### From inside the book

Results 1-3 of 56

Page 273

11.2 ( 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 ...

11.2 ( 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 ...

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 = y1 + $ 2 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 = y1 + $ 2 at an ion as the sum of two distinct but related

**potentials**.Page 572

( a ) Charge distribution used for computing

computed ( it includes the dashed curve at the reference point ) , while yo is the

( a ) Charge distribution used for computing

**potential**| ı ; the**potential**Va iscomputed ( it includes the dashed curve at the reference point ) , while yo is the

**potential**of the dashed curve alone . ( b ) Charge distribution for**potential**: The ...### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Contents

DIFFRACTION OF XRAYS BY CRYSTALS | 44 |

CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |

ELASTIC CONSTANTS OF CRYSTALS | 85 |

Copyright | |

17 other sections not shown

### Other editions - View all

### Common terms and phrases

alloys applied approximately associated atoms axes 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 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