Introduction to Solid State Physicsproblems after each chapter |
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Page 150
The total thermal resistivity W of a fairly pure metal at low temperatures ( T < / 10 )
may be written in the form 1 ( 6.57 ) W Wo + Wi K Here Wo is the thermal
resistivity due to electron scattering by lattice vibrations and W ; is the thermal
resistivity ...
The total thermal resistivity W of a fairly pure metal at low temperatures ( T < / 10 )
may be written in the form 1 ( 6.57 ) W Wo + Wi K Here Wo is the thermal
resistivity due to electron scattering by lattice vibrations and W ; is the thermal
resistivity ...
Page 239
Experimental points involving resistivity measurements of Cu and Ag films at
room temperature , shown with curves calculated from theory to obtain
approximate values of mean free paths . Here e ' is the resistivity in the film ; p is
the bulk ...
Experimental points involving resistivity measurements of Cu and Ag films at
room temperature , shown with curves calculated from theory to obtain
approximate values of mean free paths . Here e ' is the resistivity in the film ; p is
the bulk ...
Page 489
MacDonald ' has pointed out there is an apparent excess electric resistivity in Li ,
Na , and K as the melting point is approached . The excess is with respect to a
linear increase of resistivity with temperature . Results for sodium are plotted in
Fig ...
MacDonald ' has pointed out there is an apparent excess electric resistivity in Li ,
Na , and K as the melting point is approached . The excess is with respect to a
linear increase of resistivity with temperature . Results for sodium are plotted in
Fig ...
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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