Introduction to Solid State Physicsproblems after each chapter |
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Page 139
where Q is the flux of thermal energy ( energy transmitted across unit area per
unit time ) ; K is often expressed in units cal ... If the energy were propagated
directly through the specimen without deflection , then the expression for the
thermal ...
where Q is the flux of thermal energy ( energy transmitted across unit area per
unit time ) ; K is often expressed in units cal ... If the energy were propagated
directly through the specimen without deflection , then the expression for the
thermal ...
Page 431
In cubic crystals the dimensional changes may be expressed approximately by
the relation ( 15 . ... 33 ) does not give a very good fit to the observations , and an
expression involving four parameters instead of two is often used , as discussed ...
In cubic crystals the dimensional changes may be expressed approximately by
the relation ( 15 . ... 33 ) does not give a very good fit to the observations , and an
expression involving four parameters instead of two is often used , as discussed ...
Page 575
... MECHANICAL EXPRESSION FOR THE POLARIZABILITY We compute the
energy of interaction of an atomic system with an applied static electric field and
set this equal to the macroscopic expression for the energy , which is ( B . 1 ) AE ...
... MECHANICAL EXPRESSION FOR THE POLARIZABILITY We compute the
energy of interaction of an atomic system with an applied static electric field and
set this equal to the macroscopic expression for the energy , which is ( B . 1 ) AE ...
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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 neighbor 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