Introduction to Solid State Physics |
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Page 95
MEASUREMENT OF DIELECTRIC CONSTANTS The usual methods of
measuring dielectric constants are based on a comparison of the capacity ( " ' of a
condenser filled with the substance Specimen CM 2000 wo F VI ( C , + C ) Fig . 6
. 5 .
MEASUREMENT OF DIELECTRIC CONSTANTS The usual methods of
measuring dielectric constants are based on a comparison of the capacity ( " ' of a
condenser filled with the substance Specimen CM 2000 wo F VI ( C , + C ) Fig . 6
. 5 .
Page 139
METHOD OF MEASUREMENT OF SUSCEPTIBILITIES The usual methods of
measuring diamagnetic and paramagnetic susceptibilities depend in one way or
another on the force exerted on a specimen by a non - uniform magnetic field .
METHOD OF MEASUREMENT OF SUSCEPTIBILITIES The usual methods of
measuring diamagnetic and paramagnetic susceptibilities depend in one way or
another on the force exerted on a specimen by a non - uniform magnetic field .
Page 153
Electromagnet Specimen Tor - f supply and circuit for measuring losses - and
circuito de Hses Aliti Hx4 H static ) H ... The r - f power absorbed in the specimen
is determined by electrical measurements , as by measuring the Q of the coil .
Electromagnet Specimen Tor - f supply and circuit for measuring losses - and
circuito de Hses Aliti Hx4 H static ) H ... The r - f power absorbed in the specimen
is determined by electrical measurements , as by measuring the Q of the coil .
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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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