## Introduction to Solid State Physicsproblems after each chapter |

### From inside the book

Results 1-3 of 84

Page 42

Find the space group of the

the maximum proportion of the available volume which may be filled by hard

spheres arranged in various structures is Simple

Find the space group of the

**cubic**ZnS ( zinc blende ) structure . 1 . 5 . Show thatthe maximum proportion of the available volume which may be filled by hard

spheres arranged in various structures is Simple

**cubic**Body - centered**cubic**...Page 102

Show that the bulk modulus B = – V ( dp / DV ) in

+ 2012 3 4 . 4 . A

expressions for Young ' s modulus and Poisson ' s ratio in terms of the elastic ...

Show that the bulk modulus B = – V ( dp / DV ) in

**cubic**crystals is given by B - 11+ 2012 3 4 . 4 . A

**cubic**crystal is subject to tension in the [ 100 ] direction . Findexpressions for Young ' s modulus and Poisson ' s ratio in terms of the elastic ...

Page 161

The proof we have given for the vanishing of Ez actually obtains for all cases in

which the environment of the reference point is

parallel . Thus Ez = 0 for induced polarization on simple

The proof we have given for the vanishing of Ez actually obtains for all cases in

which the environment of the reference point is

**cubic**, as long as the dipoles areparallel . Thus Ez = 0 for induced polarization on simple

**cubic**, body - centered ...### 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 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