Introduction to Solid State Physics |
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Page 240
CONDUCTIVITY DATA FOR METALS AT 0°C One free electron per atom is
assumed ; A is calculated by using Eq . ( 12 . 79 ) ; values after Mott and Jones ,
with an error of a factor of 2 in their A ' s corrected . Metal Free Observed
Calculated ...
CONDUCTIVITY DATA FOR METALS AT 0°C One free electron per atom is
assumed ; A is calculated by using Eq . ( 12 . 79 ) ; values after Mott and Jones ,
with an error of a factor of 2 in their A ' s corrected . Metal Free Observed
Calculated ...
Page 262
The first calculations were made by Bloch . In the high temperature region the
calculated conductivity is proportional to T - 1 , and in the low temperature region
it is proportional to 7 - 5 . The agreement of the calculated temperature ...
The first calculations were made by Bloch . In the high temperature region the
calculated conductivity is proportional to T - 1 , and in the low temperature region
it is proportional to 7 - 5 . The agreement of the calculated temperature ...
Page 266
Reference to detailed theoretical calculations of the conductivity of metals are
given in the review by Bardeen . 13 A comparison of observed and calculated
values of the conductivity of a number of monovalent metals is reproduced from
this ...
Reference to detailed theoretical calculations of the conductivity of metals are
given in the review by Bardeen . 13 A comparison of observed and calculated
values of the conductivity of a number of monovalent metals is reproduced from
this ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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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