## Introduction to Solid State Physicsproblems after each chapter |

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Page 135

In fact the heat capacity of metals at high

different from that of insulators . ... For normal metals the definition of a low

order ...

In fact the heat capacity of metals at high

**temperatures**usually is not particularlydifferent from that of insulators . ... For normal metals the definition of a low

**temperature**for the present purpose is by comparison with a**temperature**of theorder ...

Page 242

involves neither N , m , or T . A more detailed study of the quantum theory of

transport processes in metals shows that the Lorenz number is expected to be

independent of

differences ...

involves neither N , m , or T . A more detailed study of the quantum theory of

transport processes in metals shows that the Lorenz number is expected to be

independent of

**temperature**only above the Debye**temperature**, as thedifferences ...

Page 301

Theoretical ( Grüneisen )

experimental values for various metals . ( After Bardeen . ) first quantum

calculations were made by Bloch . In the high

conductivity ...

Theoretical ( Grüneisen )

**temperature**variation of electrical resistance , andexperimental values for various metals . ( After Bardeen . ) first quantum

calculations were made by Bloch . In the high

**temperature**region the calculatedconductivity ...

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### Contents

DIFFRACTION OF XRAYS BY CRYSTALS | 44 |

CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |

ELASTIC CONSTANTS OF CRYSTALS | 85 |

Copyright | |

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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 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