## Introduction to Solid State Physicsproblems after each chapter |

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Page 42

Prove this statement by considering a vector a taken to be the smallest non -

vanishing translation of the lattice , and

shorter than a , where a ' is a vector obtained from a by a rotation of 24 / 5 . ( b )

Prove that ...

Prove this statement by considering a vector a taken to be the smallest non -

vanishing translation of the lattice , and

**show**that the vector a a ' would beshorter than a , where a ' is a vector obtained from a by a rotation of 24 / 5 . ( b )

Prove that ...

Page 180

( a )

hydrogen atom gives a = ano , where ay is the Bohr radius . ( b ) Consider a

semiclassical model of the ground state of the hydrogen atom in an electric field

normal to the ...

( a )

**Show**that the expression ( 7.14 ) applied to the first Bohr orbit of thehydrogen atom gives a = ano , where ay is the Bohr radius . ( b ) Consider a

semiclassical model of the ground state of the hydrogen atom in an electric field

normal to the ...

Page 231

susceptibility of atomic hydrogen ( -2.36 X 10-6 cm ... Given an atom with a

spherically symmetrical charge distribution in an external field H ,

field at the ...

**Show**that for this state pa 2 = 3ao ?, and calculate the molar diamagneticsusceptibility of atomic hydrogen ( -2.36 X 10-6 cm ... Given an atom with a

spherically symmetrical charge distribution in an external field H ,

**show**that thefield at the ...

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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