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 He H
, ( static ) r - f coil Fig . 9 . 7 . ... 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 He H
, ( static ) r - f coil Fig . 9 . 7 . ... The r - f power absorbed in the specimen is
determined by electrical measurements , as by measuring the Q of the coil .
Page 456
In d - c measurements the resistivity in the superconducting state is zero . ... that
of the normal state ; that is , no change in the resistivity , as measured by the
reflection coefficient , is observed on passing through the critical magnetic field .
In d - c measurements the resistivity in the superconducting state is zero . ... that
of the normal state ; that is , no change in the resistivity , as measured by the
reflection coefficient , is observed on passing through the critical magnetic field .
Page 549
Comparison of theoretical curve with measurements of relative grainboundary
energy . The theoretical curve is given by E / Em = ( 0 / 0m ) [ 1 – In ( 0 / 0m ) ] ; 0 ,
for each of the four sets of measurements is listed ; the corresponding values of ...
Comparison of theoretical curve with measurements of relative grainboundary
energy . The theoretical curve is given by E / Em = ( 0 / 0m ) [ 1 – In ( 0 / 0m ) ] ; 0 ,
for each of the four sets of measurements is listed ; the corresponding values of ...
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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 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