Introduction to Solid State Physicsproblems after each chapter |
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Page 162
When the dielectric is inserted , polarization charge densities + P are induced on the surfaces of the dielectric , and these charges are then effectively neutralized by a flow of charge around the condenser circuit .
When the dielectric is inserted , polarization charge densities + P are induced on the surfaces of the dielectric , and these charges are then effectively neutralized by a flow of charge around the condenser circuit .
Page 273
We expect the ion cores to bear a positive charge , as V. potential energy ( a ) T X ( b ) lely 1 % , charge density pelen ? l 4,1 ? Plane wave XX A lekyla Fig . 11.2 . ( a ) Variation of potential energy of a conduction electron in the ...
We expect the ion cores to bear a positive charge , as V. potential energy ( a ) T X ( b ) lely 1 % , charge density pelen ? l 4,1 ? Plane wave XX A lekyla Fig . 11.2 . ( a ) Variation of potential energy of a conduction electron in the ...
Page 571
We shall consider a lattice made up of ions with positive or negative charges and shall assume that the ions are spherical and ... The potential i is that of a structure with a Gaussian distribution of charge situated at each ion site ...
We shall consider a lattice made up of ions with positive or negative charges and shall assume that the ions are spherical and ... The potential i is that of a structure with a Gaussian distribution of charge situated at each ion site ...
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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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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 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