## Introduction to Solid State Physicsproblems after each chapter |

### From inside the book

Results 1-3 of 26

Page 150

The total thermal

10 ) may be written in the form ( 6 . 57 ) W = Wo + W ; = 7 Here Wo is the thermal

The total thermal

**resistivity**W of a fairly pure metal at low temperatures ( T < 0 /10 ) may be written in the form ( 6 . 57 ) W = Wo + W ; = 7 Here Wo is the thermal

**resistivity**due to electron scattering by lattice vibrations and W ; is the thermal ...Page 239

Experimental points involving

room temperature , shown with curves calculated from theory to obtain

approximate values of mean free paths . Here e ' is the

the bulk ...

Experimental points involving

**resistivity**measurements of Cu and Ag films atroom temperature , shown with curves calculated from theory to obtain

approximate values of mean free paths . Here e ' is the

**resistivity**in the film ; p isthe bulk ...

Page 270

Yet the distinction between the

apart , and insulators is striking : the

temperatures may be of the order of 10 - 8 ohm - cm , and the

insulator ...

Yet the distinction between the

**resistivity**values of conductors , superconductivityapart , and insulators is striking : the

**resistivity**of a pure metal at lowtemperatures may be of the order of 10 - 8 ohm - cm , and the

**resistivity**of a goodinsulator ...

### 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 neighbor 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