## Introduction to Solid State Physics |

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Page 43

The elastic constants are of interest because of the insight they

nature of the binding forces in solids , and they are also of importance for the

thermal properties of solids . We

of ...

The elastic constants are of interest because of the insight they

**give**into thenature of the binding forces in solids , and they are also of importance for the

thermal properties of solids . We

**give**first a review of the formal phenomenologyof ...

Page 88

5 . 6 . Writing Or = hw / k , find the limiting form at low temperatures of the Einstein

heat capacity ( 5 . 21 ) .

way the heat capacities on the Einstein and Debye theories approach zero . 5 .

5 . 6 . Writing Or = hw / k , find the limiting form at low temperatures of the Einstein

heat capacity ( 5 . 21 ) .

**Give**a qualitative physical reason for the difference in theway the heat capacities on the Einstein and Debye theories approach zero . 5 .

Page 162

More exact quantum statistics

lattice ( z = 6 ) with S = į various calculations

shown in most texts on quantum theory ; see also J . H . Van Vleck , Revs .

Modern ...

More exact quantum statistics

**give**somewhat different results . For a simple cubiclattice ( z = 6 ) with S = į various calculations

**give**the results below. 8 This isshown in most texts on quantum theory ; see also J . H . Van Vleck , Revs .

Modern ...

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### Contents

LATTICE ENERGY OF IONIC CRYSTALS | 29 |

ELASTIC CONSTANTS OF CRYSTALS | 43 |

LATTICE VIBRATIONS | 60 |

Copyright | |

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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero