## Introduction to Solid State Physicsproblems after each chapter |

### From inside the book

Results 1-3 of 90

Page 53

GEOMETRICAL STRUCTURE FACTOR The Laue and Bragg equations determine the reflections ( hkl ) which are possible for a

GEOMETRICAL STRUCTURE FACTOR The Laue and Bragg equations determine the reflections ( hkl ) which are possible for a

**given**crystal lattice , but the relative intensities of the various reflections depend on the contents of the unit cell ...Page 94

2 дх2 az2 av + ( C12 + C44 ) aw + ах дz , дх ду One solution is

2 дх2 az2 av + ( C12 + C44 ) aw + ах дz , дх ду One solution is

**given**by a longitudinal wave , U oei ( wt - ko ) , U = moving along the x cube edge ; from ( 4.25 ) -wapo - koc11 , so that the velocity is ( 4.26 ) v = w / k = ( cu / po ) ...Page 216

This equation for an electron spin with g = 2 appears to differ from the classical result ( 9.14 ) by a factor of 3 ; however , in quantum mechanics the total spin angular momentum is

This equation for an electron spin with g = 2 appears to differ from the classical result ( 9.14 ) by a factor of 3 ; however , in quantum mechanics the total spin angular momentum is

**given**by ( S ( S + 1 ) ] ” = ( ) } 4 rather than by ...### 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 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