Introduction to Solid State Physicsproblems after each chapter |
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Page 225
The Electromagnet Specimen Tor - f supply and circuit for measuring losses Hz H
, ( static ) r - f coil Fig . 9.7 . Schematic ... The r - f power absorbed in the specimen
is determined by electrical measurements , as by measuring the Q of the coil .
The Electromagnet Specimen Tor - f supply and circuit for measuring losses Hz H
, ( static ) r - f coil Fig . 9.7 . Schematic ... The r - f power absorbed in the specimen
is determined by electrical measurements , as by measuring the Q of the coil .
Page 471
The field Hi will exceed the critical field Hc ( as determined from measurements
on a long wire in an axial field ) when ( 16.48 ) H > Hc 3 When this situation
occurs we can avoid having the whole sphere become normal by having the
material ...
The field Hi will exceed the critical field Hc ( as determined from measurements
on a long wire in an axial field ) when ( 16.48 ) H > Hc 3 When this situation
occurs we can avoid having the whole sphere become normal by having the
material ...
Page 549
Comparison of theoretical curve with meăsurements of relative grainboundary
energy . ... Om for each of the four sets of measurements is listed ; the
corresponding values of Em are not known , since only relative energies are
measured .
Comparison of theoretical curve with meăsurements of relative grainboundary
energy . ... Om for each of the four sets of measurements is listed ; the
corresponding values of Em are not known , since only relative energies are
measured .
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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