## Introduction to Solid State Physicsproblems after each chapter |

### From inside the book

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Page 96

If then a cubic crystal were elastically isotropic and the Cauchy

the velocity of the transverse waves would be equal to ( 3 ) ” the velocity of the

longitudinal waves . The conditions for the validity of the Cauchy

If then a cubic crystal were elastically isotropic and the Cauchy

**relation**satisfied ,the velocity of the transverse waves would be equal to ( 3 ) ” the velocity of the

longitudinal waves . The conditions for the validity of the Cauchy

**relations**are : 1 .Page 244

This is the celebrated de Broglie

practical

units ( 10 - 8 cm ) and V is the accelerating voltage in volts . We see that the ...

This is the celebrated de Broglie

**relation**. The wave nature of ... A convenientpractical

**relation**for electrons is ( A ) = ( 150 / V ) , where 1 is given in Angstromunits ( 10 - 8 cm ) and V is the accelerating voltage in volts . We see that the ...

Page 612

... 27 translation , 1 Group velocity , 288 Growth spirals in crystals , 562

Grüneisen formula , electrical conductivity , 301 , 304 Grüneisen

Gurney - Mott theory of photographic process , 500 Gyromagnetic experiments ,

408 , 410 F ...

... 27 translation , 1 Group velocity , 288 Growth spirals in crystals , 562

Grüneisen formula , electrical conductivity , 301 , 304 Grüneisen

**relation**, 154Gurney - Mott theory of photographic process , 500 Gyromagnetic experiments ,

408 , 410 F ...

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### Contents

DIFFRACTION OF XRAYS BY CRYSTALS | 44 |

CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |

ELASTIC CONSTANTS OF CRYSTALS | 85 |

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### 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