## Introduction to Solid State Physicsproblems after each chapter |

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Page 53

GEOMETRICAL STRUCTURE FACTOR The Laue and Bragg equations

determine the reflections ( hkl ) which are possible for a

the relative intensities of the various reflections depend on the contents of the unit

cell ...

GEOMETRICAL STRUCTURE FACTOR The Laue and Bragg equations

determine the reflections ( hkl ) which are possible for a

**given**crystal lattice , butthe relative intensities of the various reflections depend on the contents of the unit

cell ...

Page 94

9 ) , to ( 42 ) noi - en nat cu C + ) C aʼw dx dz / lamat7 ay + ( C12 + C44 ) ( \ дах

ду One solution is

the x cube edge ; from ( 4 . 25 ) - wapo = – k ? c11 , so that the velocity is ( 4 .

9 ) , to ( 42 ) noi - en nat cu C + ) C aʼw dx dz / lamat7 ay + ( C12 + C44 ) ( \ дах

ду One solution is

**given**by a longitudinal wave , u = unei ( wl ka ) . moving alongthe x cube edge ; from ( 4 . 25 ) - wapo = – k ? c11 , so that the velocity is ( 4 .

Page 487

Charles Kittel. vacancies is independent of temperature , and the slope of the plot

of log o vs . 1 / kt gives essentially E + , the barrier activitation energy for the

jumping of positive ion vacancies . Representative values of Et are

17 ...

Charles Kittel. vacancies is independent of temperature , and the slope of the plot

of log o vs . 1 / kt gives essentially E + , the barrier activitation energy for the

jumping of positive ion vacancies . Representative values of Et are

**given**in Table17 ...

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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