## Introduction to Solid State Physicsproblems after each chapter |

### From inside the book

Results 1-3 of 92

Page 46

It should be emphasized that the Bragg

periodicity of the structure , and the

composition or arrangement of the atoms associated with the reflecting planes .

The latter ...

It should be emphasized that the Bragg

**equation**results from the fundamentalperiodicity of the structure , and the

**equation**does not refer to the actualcomposition or arrangement of the atoms associated with the reflecting planes .

The latter ...

Page 245

In this

, which is constant . The function is the wave function or eigenfunction , and has

the significance that , when properly normalized , ** dx dy dz is the probability of ...

In this

**equation**3 ? 02 D2 82 + ду ? + 2.x2 azzi h h / 27 ; and E is the total energy, which is constant . The function is the wave function or eigenfunction , and has

the significance that , when properly normalized , ** dx dy dz is the probability of ...

Page 613

... superconductivity , 156 Local fields , perovskite structure , 192 London

213 Langevin ...

... superconductivity , 156 Local fields , perovskite structure , 192 London

**equations**, superconductivity , 464 Long range ... 215 Langevin - Debye**equation**, 171 Langevin diamagnetism ,**equation**, 207 Langevin function , 170 ,213 Langevin ...

### 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 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 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