Introduction to Solid State Physicsproblems after each chapter |
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Page 207
DIAMAGNETISM Substances with a negative magnetic susceptibility are called diamagnetic . Substances with a positive susceptibility are called paramagnetic . The magnetic susceptibility per unit volume is defined as x = M / H , where M ...
DIAMAGNETISM Substances with a negative magnetic susceptibility are called diamagnetic . Substances with a positive susceptibility are called paramagnetic . The magnetic susceptibility per unit volume is defined as x = M / H , where M ...
Page 220
2 netic field in the z direction the orbital contribution to the magnetic moment is proportional to the expectation value of L2 , and so the orbital magnetic moment is quenched if the mechanical moment L , is quenched .
2 netic field in the z direction the orbital contribution to the magnetic moment is proportional to the expectation value of L2 , and so the orbital magnetic moment is quenched if the mechanical moment L , is quenched .
Page 296
When a conductor is placed in a magnetic field perpendicular to the direction of current flow , a voltage is developed across the specimen in the direction perpendicular to both the current Us + + + + + + + + + Ey H , Fig . 11.14 .
When a conductor is placed in a magnetic field perpendicular to the direction of current flow , a voltage is developed across the specimen in the direction perpendicular to both the current Us + + + + + + + + + Ey H , Fig . 11.14 .
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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 present 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