## Solid State PhysicsThis book provides an introduction to the field of solid state physics for undergraduate students in physics, chemistry, engineering, and materials science. |

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Page 217

Thus if Ak measures the region within which g ( and hence ğ ) is appreciable , "

then „ ro + R ) , in accordance with the usual rules for wave packets , should be

appreciable within a region of dimensions AR = 1 / Ak . Since Ak is small

Thus if Ak measures the region within which g ( and hence ğ ) is appreciable , "

then „ ro + R ) , in accordance with the usual rules for wave packets , should be

appreciable within a region of dimensions AR = 1 / Ak . Since Ak is small

**compared**...Page 359

The quantity of charge that must be redistributed among the surfaces to produce

such exterior fields is minute ,

redistributed among neighboring surface cells in establishing the double layer .

The quantity of charge that must be redistributed among the surfaces to produce

such exterior fields is minute ,

**compared**with the amount of charge that isredistributed among neighboring surface cells in establishing the double layer .

Page 618

Evidently this will yield an Fo , which is the equilibrium potential energy of the

lattice with vacancies plus the free energy of the phonons Fo = Ujeq + Fph . ( 30 .

9 ) The second term is generally small

Evidently this will yield an Fo , which is the equilibrium potential energy of the

lattice with vacancies plus the free energy of the phonons Fo = Ujeq + Fph . ( 30 .

9 ) The second term is generally small

**compared**with the first , so that to a first ...### What people are saying - Write a review

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### Contents

The Drude Theory of Metals | 1 |

Free electron densities and ra | 5 |

Thermal conductivities | 21 |

Copyright | |

46 other sections not shown

### Other editions - View all

Solid State Physics: Advances in Research and Applications, Volume 42 Henry Ehrenreich Limited preview - 1989 |

### Common terms and phrases

additional applied approximation assume atomic band boundary Bragg Bravais lattice calculation carrier Chapter charge close collisions compared completely condition conduction consider constant containing contribution correction crystal cubic density dependence derivation described determined direction discussion distribution effect electric field elements energy equal equation equilibrium example fact Fermi surface Figure follows free electron frequency given gives heat hexagonal holes important independent integral interaction ionic ions known lattice vector leading levels limit linear magnetic field mean measured metals method momentum motion normal Note observed occupied orbits perpendicular phonon plane positive possible potential present primitive cell problem properties reciprocal lattice reflection region relation requires result satisfy scattering semiclassical Show shown simple single solid solution space specific structure symmetry Table temperature term theory thermal vanishes volume wave functions wave vector zero zone