Introduction to Solid State Physics |
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Page 89
The polarization is defined as the dipole moment per unit volume , the dipole
moment P 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 polarization is defined as the dipole moment per unit volume , the dipole
moment P 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 ...
Page 90
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 171
The behavior observed in single crystals is similar to that in polycrystalline
specimens . ... The increase in the value of the resultant magnetic moment of the
specimen under the action of an applied magnetic field may be imagined to take
place ...
The behavior observed in single crystals is similar to that in polycrystalline
specimens . ... The increase in the value of the resultant magnetic moment of the
specimen under the action of an applied magnetic field may be imagined to take
place ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero