Introduction to Solid State Physicsproblems after each chapter |
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Page 118
REVIEW OF CLASSICAL STATISTICAL MECHANICS The elementary result
which we remember from the theory of the ideal gas and from classical statistics
is that the average energy of a classical system is equal to jkT per degree of
freedom ...
REVIEW OF CLASSICAL STATISTICAL MECHANICS The elementary result
which we remember from the theory of the ideal gas and from classical statistics
is that the average energy of a classical system is equal to jkT per degree of
freedom ...
Page 180
The correct quantum - mechanical result is larger than this by the factor g . 7 . 2 .
In the local field problem the cavity need not be chosen as spherical , but may be
of any shape possessing at least cubic symmetry . We may for example take the ...
The correct quantum - mechanical result is larger than this by the factor g . 7 . 2 .
In the local field problem the cavity need not be chosen as spherical , but may be
of any shape possessing at least cubic symmetry . We may for example take the ...
Page 591
It is a well - known thermodynamic results that the condition for two phases to be
in equilibrium with respect to any chemical ... This result follows on considering
the change of the Helmholtz free energy ( N . 9 ) dF = - pdV – SAT – Eu dn on ...
It is a well - known thermodynamic results that the condition for two phases to be
in equilibrium with respect to any chemical ... This result follows on considering
the change of the Helmholtz free energy ( N . 9 ) dF = - pdV – SAT – Eu dn on ...
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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