## Introduction to Solid State Physicsproblems after each chapter |

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Page 43

I. , G. Bell and Sons , Ltd. ,

crystallography , John Wiley & Sons , New York , 1956 . C. W. Bunn , Chemical

crystallography , Clarendon Press , Oxford , 1945 . P. H. Groth , Chemische

Krystallographie ...

I. , G. Bell and Sons , Ltd. ,

**London**, 1933 . M. J. Buerger , Elementarycrystallography , John Wiley & Sons , New York , 1956 . C. W. Bunn , Chemical

crystallography , Clarendon Press , Oxford , 1945 . P. H. Groth , Chemische

Krystallographie ...

Page 465

F. and H.

abandoned , and that we should take instead as the fundamental equation (

16.22 ) c curl Aj which is postulated to replace Ohm's law in superconductors .

We note ...

F. and H.

**London**17 therefore suggested that the acceleration equation beabandoned , and that we should take instead as the fundamental equation (

16.22 ) c curl Aj which is postulated to replace Ohm's law in superconductors .

We note ...

Page 467

We see then that the transition in behavior occurs when the skin depth for eddy

currents is equal to the

place when w ~ 1011 sec - , or f = 1010 cps , which is in the microwave region , in

...

We see then that the transition in behavior occurs when the skin depth for eddy

currents is equal to the

**London**penetration depth ( 16.31 ) . The transition takesplace when w ~ 1011 sec - , or f = 1010 cps , which is in the microwave region , in

...

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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 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