## Introduction to Solid State Physicsproblems after each chapter |

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Page 323

We shall usually shut our eyes to any change caused by alloying in the energy

gap at the zone

eigenvalues . We assume in fact that the lattice still possesses translational

symmetry ...

We shall usually shut our eyes to any change caused by alloying in the energy

gap at the zone

**boundary**and in the nature of the wave functions and energyeigenvalues . We assume in fact that the lattice still possesses translational

symmetry ...

Page 423

The coercive force in “ magnetically soft ” ( low H . ) materials may be understood

from the following : The total energy of a given specimen may vary with the

position of a domain

The coercive force in “ magnetically soft ” ( low H . ) materials may be understood

from the following : The total energy of a given specimen may vary with the

position of a domain

**boundary**because of local variations in internal strains ...Page 549

7 ) gives the elastic strain energy per unit length of dislocation in the

( G62 / 47 ( 1 – v ) ] In ( aD / b ) , where r , has been set equal to b and a is a

number near 1 . DE ou pou • Dunn silicon iron ( 110 ) series , Om = 26 . 6° A

Dunn ...

7 ) gives the elastic strain energy per unit length of dislocation in the

**boundary**as( G62 / 47 ( 1 – v ) ] In ( aD / b ) , where r , has been set equal to b and a is a

number near 1 . DE ou pou • Dunn silicon iron ( 110 ) series , Om = 26 . 6° A

Dunn ...

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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