Introduction to Solid State Physicsproblems after each chapter |
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Page 159
The constant N is known as the depolarization factor ; it is precisely the same as the demagnetization factor , and its value depends on the axial 1.0 0.8 0.6 1 N / 4T 0.4 1 0.2 0 1 2 5 6 3 c / a Fig . 7.2 . Demagnetization factor N ...
The constant N is known as the depolarization factor ; it is precisely the same as the demagnetization factor , and its value depends on the axial 1.0 0.8 0.6 1 N / 4T 0.4 1 0.2 0 1 2 5 6 3 c / a Fig . 7.2 . Demagnetization factor N ...
Page 237
We expect the charge transported to be proportional to the charge density Ne ; the factor elm enters because the acceleration in a given electric field is proportional to e and inversely proportional to the mass m ; the time + describes ...
We expect the charge transported to be proportional to the charge density Ne ; the factor elm enters because the acceleration in a given electric field is proportional to e and inversely proportional to the mass m ; the time + describes ...
Page 322
The size factor is somewhat unfavorable in the Cu ( 2.55 A ) – Cd ( 2.97 A ) system and only 1.7 atomic percent ... The size factors expressed as percentages referred to copper are 4 percent for Zn in Cu and 16.5 percent for Cd in Cu .
The size factor is somewhat unfavorable in the Cu ( 2.55 A ) – Cd ( 2.97 A ) system and only 1.7 atomic percent ... The size factors expressed as percentages referred to copper are 4 percent for Zn in Cu and 16.5 percent for Cd in Cu .
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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