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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 . The field E inside the needle ...
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 . The field E inside the needle ...
Page 273
We expect the ion cores to bear a positive charge , as V , potential energy ( a )
lely 12 , charge density XXXXXXX Plane wave Kl ? Fig . 11.2 . ( a ) Variation of
potential energy of a conduction electron in the field of the positive ion cores of a
...
We expect the ion cores to bear a positive charge , as V , potential energy ( a )
lely 12 , charge density XXXXXXX Plane wave Kl ? Fig . 11.2 . ( a ) Variation of
potential energy of a conduction electron in the field of the positive ion cores of a
...
Page 522
n where n is the surface concentration of free charge . In this estimate we are
taking the dielectric constant of the crystal as unity . Thus n = 1 / 4we = 2 X 108
electrons cm ? This figure is comparable with the amount of charge piled up by a
...
n where n is the surface concentration of free charge . In this estimate we are
taking the dielectric constant of the crystal as unity . Thus n = 1 / 4we = 2 X 108
electrons cm ? This figure is comparable with the amount of charge piled up by a
...
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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 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
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Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials, ISSN 0084-0203 Wiley series on the science and technology of materials. J. H. Hollomon, advisory editor |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1956 |
| Original from | the University of California |
| Digitized | 21 Sep 2007 |
| ISBN | 0852264674, 9780852264676 |
| Length | 617 pages |
| Export Citation | BiBTeX EndNote RefMan |