## Introduction to Solid State Physics |

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Page 14

In

same indices , but this is not generally true in other crystal systems . The

positions of points in a unit cell are specified in terms of lattice coordinates , in

which ...

In

**cubic**crystals a direction [ uvw ] is perpendicular to a plane ( uvw ) having thesame indices , but this is not generally true in other crystal systems . The

positions of points in a unit cell are specified in terms of lattice coordinates , in

which ...

Page 27

Show that the maximum proportion of the available volume which may be filled

by hard spheres arranged in various structures is Simple

Show that the maximum proportion of the available volume which may be filled

by hard spheres arranged in various structures is Simple

**cubic**Body - centered**cubic**Face - centered**cubic**Hexagonal close - packed Diamond a / 6 ( = 0 .Page 59

Show that the bulk modulus B = - V ( dp / dV ) in

C11 + 2012 3 . 4 . A

Find expressions for Young ' s modulus and Poisson ' s ratio in terms of the

elastic ...

Show that the bulk modulus B = - V ( dp / dV ) in

**cubic**crystals is given by B =C11 + 2012 3 . 4 . A

**cubic**crystal is subject to tension in the ( 100 ) direction .Find expressions for Young ' s modulus and Poisson ' s ratio in terms of the

elastic ...

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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