Introduction to Solid State Physics |
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Page 85
5 ) decreases as the temperature is lowered ; this effect is present even at room
temperature . Furthermore , the values of the thermal conductivity at room
temperature run about an order of magnitude lower for glasses than for ( De
Haas ...
5 ) decreases as the temperature is lowered ; this effect is present even at room
temperature . Furthermore , the values of the thermal conductivity at room
temperature run about an order of magnitude lower for glasses than for ( De
Haas ...
Page 206
The superconducting elements and their transition temperatures are listed in
Table 11 . 1 . ... For example ; titanium , zirconium , and hafnium have resistivities
at room temperature of 89 , 45 , and 32 microhm - cm , respectively , while copper
...
The superconducting elements and their transition temperatures are listed in
Table 11 . 1 . ... For example ; titanium , zirconium , and hafnium have resistivities
at room temperature of 89 , 45 , and 32 microhm - cm , respectively , while copper
...
Page 246
At room temperature the values observed are in fair 50 mm TTTTTT 712 Thermal
conductivity ( watts / cm deg ) ( cal / sec cm deg ) os 20 - 40 - 60 - 80 - 100 °
Temperature ( °K ) Fig . 12 . 6 . The thermal conductivity of copper . ( After
Berman ...
At room temperature the values observed are in fair 50 mm TTTTTT 712 Thermal
conductivity ( watts / cm deg ) ( cal / sec cm deg ) os 20 - 40 - 60 - 80 - 100 °
Temperature ( °K ) Fig . 12 . 6 . The thermal conductivity of copper . ( After
Berman ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero