## Introduction to Solid State Physicsproblems after each chapter |

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Page 83

There are in general six orders and eight combinations of sign , making forty -

eight

there are ...

There are in general six orders and eight combinations of sign , making forty -

eight

**equivalent**positions . If one of the n ' s is zero , there are twenty - four**equivalent**positions . If two n ' s are**equal**in magnitude but different from zero ,there are ...

Page 180

Note : If the applied field is in the x direction , then the x component of the field of

the nucleus at the displaced position of the electron orbit must be

applied field . The correct quantum - mechanical result is larger than this by the ...

Note : If the applied field is in the x direction , then the x component of the field of

the nucleus at the displaced position of the electron orbit must be

**equal**to theapplied field . The correct quantum - mechanical result is larger than this by the ...

Page 341

When S = 0 , each lattice contains

no long range order . We consider now that part of the internal energy associated

with AA , AB , and BB nearest neighbor bond energies , with the ultimate object ...

When S = 0 , each lattice contains

**equal**numbers of A and B atoms and there isno long range order . We consider now that part of the internal energy associated

with AA , AB , and BB nearest neighbor bond energies , with the ultimate object ...

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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 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