## Introduction to Solid State Physicsproblems after each chapter |

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Page 118

REVIEW OF CLASSICAL STATISTICAL MECHANICS The elementary

which we remember from the theory of the ideal gas and from classical statistics

is that the average energy of a classical system is equal to jkT per degree of

freedom ...

REVIEW OF CLASSICAL STATISTICAL MECHANICS The elementary

**result**which we remember from the theory of the ideal gas and from classical statistics

is that the average energy of a classical system is equal to jkT per degree of

freedom ...

Page 180

The correct quantum - mechanical

In the local field problem the cavity need not be chosen as spherical , but may be

of any shape possessing at least cubic symmetry . We may for example take the ...

The correct quantum - mechanical

**result**is larger than this by the factor g . 7 . 2 .In the local field problem the cavity need not be chosen as spherical , but may be

of any shape possessing at least cubic symmetry . We may for example take the ...

Page 591

It is a well - known thermodynamic

in equilibrium with respect to any chemical ... This

the change of the Helmholtz free energy ( N . 9 ) dF = - pdV – SAT – Eu dn on ...

It is a well - known thermodynamic

**results**that the condition for two phases to bein equilibrium with respect to any chemical ... This

**result**follows on consideringthe change of the Helmholtz free energy ( N . 9 ) dF = - pdV – SAT – Eu dn on ...

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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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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