Introduction to Solid State Physicsproblems after each chapter |
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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 Vx + + + + + Еу H , Fig . 11.14 . Hall effect .
Electrons ...
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 Vx + + + + + Еу H , Fig . 11.14 . Hall effect .
Electrons ...
Page 402
Let us postulate such an interaction and call it the Weiss field . The orienting
effect of the Weiss field is opposed by the motion of thermal agitation of the
elementary moments . We consider the Weiss field the equivalent of an effective
magnetic ...
Let us postulate such an interaction and call it the Weiss field . The orienting
effect of the Weiss field is opposed by the motion of thermal agitation of the
elementary moments . We consider the Weiss field the equivalent of an effective
magnetic ...
Page 452
The currents have been observed by the associated magnetic field to persist with
undiminished strength for days . In experiments at Leiden using a coil of 700
meters of lead wire wound non - inductively it was impossible in a run of about 12
hr ...
The currents have been observed by the associated magnetic field to persist with
undiminished strength for days . In experiments at Leiden using a coil of 700
meters of lead wire wound non - inductively it was impossible in a run of about 12
hr ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
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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