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 .
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 .
Page 242
At room temperature the values observed are in quite good agreement with the theoretical value given in ( 10.22 ) , as shown in Table 10.2 . The Lorenz number of pure copper at liquid hydrogen temperature ( ~ 15 ° K ) is an order of ...
At room temperature the values observed are in quite good agreement with the theoretical value given in ( 10.22 ) , as shown in Table 10.2 . The Lorenz number of pure copper at liquid hydrogen temperature ( ~ 15 ° K ) is an order of ...
Page 459
The superconducting elements and their transition temperatures are listed in Table 16.1 . ... ( c ) Superconducting metals are not as good conductors at room temperature as the normal metals at room temperature .
The superconducting elements and their transition temperatures are listed in Table 16.1 . ... ( c ) Superconducting metals are not as good conductors at room temperature as the normal metals at room temperature .
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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 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