Introduction to Solid State Physicsproblems after each chapter |
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Page 157
The polarization is defined as the dipole moment per unit volume , the dipole
moment of the specimen as a whole being defined as P = Seifi . The sum is
extended over all charges in the system ; on the supposition that the system is
neutral the ...
The polarization is defined as the dipole moment per unit volume , the dipole
moment of the specimen as a whole being defined as P = Seifi . The sum is
extended over all charges in the system ; on the supposition that the system is
neutral the ...
Page 158
If we are far enough away from the individual dipoles of a uniformly polarized
specimen , we may , according to an elementary transformation occurring in
electrostatic theory , calculate the field of the specimen as equal to the field of a
surface ...
If we are far enough away from the individual dipoles of a uniformly polarized
specimen , we may , according to an elementary transformation occurring in
electrostatic theory , calculate the field of the specimen as equal to the field of a
surface ...
Page 409
-Suspension The two principal gyromagnetic methods are ( 1 ) the Einstein - de
Haas method , in which one reverses the magnetization of a freely suspended
specimen and observes the resulting rotation ; and ( 2 ) the Barnett method , in ...
-Suspension The two principal gyromagnetic methods are ( 1 ) the Einstein - de
Haas method , in which one reverses the magnetization of a freely suspended
specimen and observes the resulting rotation ; and ( 2 ) the Barnett method , in ...
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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