## 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 ikT 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 ikT per degree of

freedom; ...

Page 180

The correct quantum-mechanical

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 \. 7.2. Inthe 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

This

dF = -v dV - SdT -2m dn on transferring dn particles from phase i to phase j at

constant volume and temperature: (N.10) dF = -nj dn + m dn. For equilibrium dF =

0, ...

This

**result**follows on considering the change of the Hclmholtz free energy (N.9)dF = -v dV - SdT -2m dn on transferring dn particles from phase i to phase j at

constant volume and temperature: (N.10) dF = -nj dn + m dn. For equilibrium dF =

0, ...

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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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absorption acceptors alkali alloy approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point levels low temperatures magnetic field metals molecules motion nearest neighbor normal observed orbital p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc recombination region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero