## Introduction to Solid State Physicsproblems after each chapter |

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Page 85

of single crystals . The

give into the nature of the binding forces in solids , and they are also of ...

**Elastic**Constants of Crystals This chapter is concerned with the**elastic**constantsof single crystals . The

**elastic**constants are of interest because of the insight theygive into the nature of the binding forces in solids , and they are also of ...

Page 92

of

crystal classes has been given by Hearmon . In Fig . 4 . 3 the experimental values

of the

of

**elastic**constant data and of relationships among various coefficients for thecrystal classes has been given by Hearmon . In Fig . 4 . 3 the experimental values

of the

**elastic**constants of sodium chloride are plotted over a wide temperature ...Page 102

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

a shear wave moving along a ( 110 ) direction with particle motion along a [ 110 ]

...

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

**elastic**compliances or stiffnesses . 4 . 5 . Show that the velocity of propagation ofa shear wave moving along a ( 110 ) direction with particle motion along a [ 110 ]

...

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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 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