## Introduction to Solid State Physicsproblems after each chapter. |

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Page 252

The classical distribution is a good approximation to the true state of affairs only

when the average spacing between

Broglie wavelength (10.24) calculated using the thermal velocity of the

The classical distribution is a good approximation to the true state of affairs only

when the average spacing between

**particles**is large in comparison with the deBroglie wavelength (10.24) calculated using the thermal velocity of the

**particles**.Page 424

sufficiently small

single domain is a result of domain theory which has been confirmed by

experiment. It can be shown82 that with such very small

a ...

sufficiently small

**particle**, with diameter less than 10 or 10 cm, is composed of asingle domain is a result of domain theory which has been confirmed by

experiment. It can be shown82 that with such very small

**particles**the formation ofa ...

Page 560

This process is followed in the hardening of steel, where

are precipitated into iron, and in hardening aluminum, where

are precipitated. If L is the mean spacing of

This process is followed in the hardening of steel, where

**particles**of iron carbideare precipitated into iron, and in hardening aluminum, where

**particles**of AI2CUare precipitated. If L is the mean spacing of

**particles**on a slip plane, the stress ...### What people are saying - Write a review

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### Contents

DIFFRACTION OF XRAYS BY CRYSTALS | 44 |

CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |

ELASTIC CONSTANTS OF CRYSTALS | 85 |

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### Common terms and phrases

absorption acceptors alkali alloy approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point levels low temperatures magnetic field metals molecules motion nearest neighbor normal observed orbital p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc recombination region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero