## Introduction to Solid State Physicsproblems after each chapter |

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Page 108

The

required , with a maximum for n = N / 2 . The

has u o sin na , permitting no motion at all , because sin ni vanishes at each ...

The

**solution**for k = 1 / L has u o sin nga / L and vanishes for n = 0 ) and n = N asrequired , with a maximum for n = N / 2 . The

**solution**for k = N * / L = a / a = kmhas u o sin na , permitting no motion at all , because sin ni vanishes at each ...

Page 236

or , if vp ( 0 ) is the initial drift velocity in the non - equilibrium distribution , the

approach to equilibrium is described by the appropriate

. 4 ) vo ( t ) = vd ( 0 ) e - t / T . We have thus arranged things so that a disturbance

...

or , if vp ( 0 ) is the initial drift velocity in the non - equilibrium distribution , the

approach to equilibrium is described by the appropriate

**solution**of ( 10 . 3 ) : ( 10. 4 ) vo ( t ) = vd ( 0 ) e - t / T . We have thus arranged things so that a disturbance

...

Page 322

BINARY ALLOYS We are now concerned primarily with substitutional solid

very restricted if the atomic diameters of solvent and solute differ by more than 15

...

BINARY ALLOYS We are now concerned primarily with substitutional solid

**solutions**of one metal in another . ... He suggests that the solid**solution**range isvery restricted if the atomic diameters of solvent and solute differ by more than 15

...

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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