## Introduction to Solid State Physicsproblems after each chapter |

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Page 94

Another solution is

edge , with the particle motion in the x direction : u = uni ( wt - ky ) , which gives ,

on substitution in ( 1.25 ) , -w po = -k % C44 , so that ( 4.27 ) V = ( C44 / po ) .

Another solution is

**given**by a transverse or shear wave moving along the y cubeedge , with the particle motion in the x direction : u = uni ( wt - ky ) , which gives ,

on substitution in ( 1.25 ) , -w po = -k % C44 , so that ( 4.27 ) V = ( C44 / po ) .

Page 257

6 ( IT ) ?, where the definite integral is

10.75 ) I = = $ o * ( E ) F " ( E ) dE = F ( Ep ) + ( kiT ) * F " ' ( Ep ) + 6 The number of

electrons is

that ...

6 ( IT ) ?, where the definite integral is

**given**in standard tables . Finally , 7 ? (10.75 ) I = = $ o * ( E ) F " ( E ) dE = F ( Ep ) + ( kiT ) * F " ' ( Ep ) + 6 The number of

electrons is

**given**by setting ( using ( 10.47 ) ] ( 10.76 ) F ( F ) = . * 5 ( E ) dE , sothat ...

Page 487

Representative values of E + are

frequency v + as arted ( 17.19 ) V + -Ex / kT vote it is found that Vot has a value

close to 1014 sec : -1 for NaCl and KCI . One expects atomic vibrational

frequencies ...

Representative values of E + are

**given**in Table 17.1 . If we express the jumpfrequency v + as arted ( 17.19 ) V + -Ex / kT vote it is found that Vot has a value

close to 1014 sec : -1 for NaCl and KCI . One expects atomic vibrational

frequencies ...

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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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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 magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential 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