Introduction to Solid State Physicsproblems after each chapter |
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Page 252
A one - particle state of the free particle system is determined by a specification of
the values of the quantum numbers nz ... This is very different from the Maxwell -
Boltzmann case where any number of particles can have the identical energy ...
A one - particle state of the free particle system is determined by a specification of
the values of the quantum numbers nz ... This is very different from the Maxwell -
Boltzmann case where any number of particles can have the identical energy ...
Page 424
sufficiently small particle , with diameter less than 10-4 or 10-5 cm , is composed
of a single domain is a result of domain theory which has been confirmed by
experiment . It can be shown22 that with such very small particles the formation of
a ...
sufficiently small particle , with diameter less than 10-4 or 10-5 cm , is composed
of a single domain is a result of domain theory which has been confirmed by
experiment . It can be shown22 that with such very small particles the formation of
a ...
Page 560
This process is followed in the hardening of steel , where particles of iron carbide
are precipitated into iron , and in hardening aluminum , where particles of Al , Cu
are precipitated . If L is the mean spacing of particles on a slip plane , the stress ...
This process is followed in the hardening of steel , where particles of iron carbide
are precipitated into iron , and in hardening aluminum , where particles of Al , Cu
are precipitated . If L is the mean spacing of particles on a slip plane , the stress ...
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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