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 . 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 208
In terms of the mean square distance p = x2 + y2 + z3 from the nucleus , we have
( 9.4 ) m2 op ? for a distribution of charge which on the average is spherically
symmetrical , so that x ? y = 7 ? Then the diamagnetic susceptibility per unit
volume ...
In terms of the mean square distance p = x2 + y2 + z3 from the nucleus , we have
( 9.4 ) m2 op ? for a distribution of charge which on the average is spherically
symmetrical , so that x ? y = 7 ? Then the diamagnetic susceptibility per unit
volume ...
Page 521
... as shown in Fig . 18.11 . SPACE CHARGE OR POLARIZATION EFFECTS i
When the illumination is not uniform throughout the crystal or when the
electrodes cannot supply or drain off charge carriers freely in the crystal , space
charges ...
... as shown in Fig . 18.11 . SPACE CHARGE OR POLARIZATION EFFECTS i
When the illumination is not uniform throughout the crystal or when the
electrodes cannot supply or drain off charge carriers freely in the crystal , space
charges ...
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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