Introduction to Solid State Physicsproblems after each chapter |
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Page 145
Temperature dependence of the thermal conductivity of various crystals and
glasses . In glasses the thermal conductivity ( Fig . 6.12 ) decreases as the
temperature is lowered ; this effect is present even at room temperature .
Furthermore , the ...
Temperature dependence of the thermal conductivity of various crystals and
glasses . In glasses the thermal conductivity ( Fig . 6.12 ) decreases as the
temperature is lowered ; this effect is present even at room temperature .
Furthermore , the ...
Page 242
At room temperature the values observed are in quite good agreement with the
theoretical value given in ( 10.22 ) , as ... of pure copper at liquid hydrogen
temperature ( ~ 15 ° K ) is an order of magnitude smaller than at room
temperature .
At room temperature the values observed are in quite good agreement with the
theoretical value given in ( 10.22 ) , as ... of pure copper at liquid hydrogen
temperature ( ~ 15 ° K ) is an order of magnitude smaller than at room
temperature .
Page 362
It is seen that for temperatures between liquid air and room temperature the
donors are essentially all ionized . Thus crystal 55 has 8 X 1012 excess donors
per cm ' , while crystal 54 has 7 x 1015 excess donors per cm . A little above room
...
It is seen that for temperatures between liquid air and room temperature the
donors are essentially all ionized . Thus crystal 55 has 8 X 1012 excess donors
per cm ' , while crystal 54 has 7 x 1015 excess donors per cm . A little above room
...
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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