Introduction to Solid State Physicsproblems after each chapter |
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Page 240
The results of more careful calculations are given in Table 10.1 . TABLE 10.1 . CONDUCTIVITY DATA FOR METALS AT 0 ° C One free electron per atom is assumed : A is calculated by using Eq . ( 10.17 ) ; values after Mott and Jones ...
The results of more careful calculations are given in Table 10.1 . TABLE 10.1 . CONDUCTIVITY DATA FOR METALS AT 0 ° C One free electron per atom is assumed : A is calculated by using Eq . ( 10.17 ) ; values after Mott and Jones ...
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Calculated values are also given in the table , using effective masses m * . The concept of an effective mass is discussed in the next chapter . TABLE 10.6 . ULTRAVIOLET TRANSMISSION OF ALKALIS K Rb Cs do ( calculated , free electrons ...
Calculated values are also given in the table , using effective masses m * . The concept of an effective mass is discussed in the next chapter . TABLE 10.6 . ULTRAVIOLET TRANSMISSION OF ALKALIS K Rb Cs do ( calculated , free electrons ...
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observed and calculated values of the conductivity of a number of monovalent metals is reproduced from this paper in Table 11.3 . The TABLE 11.3 . COMPARISON OF OBSERVED AND CALCULATED VALUES OF THE ELECTRICAL CONDUCTIVITY AT 0 ° C ...
observed and calculated values of the conductivity of a number of monovalent metals is reproduced from this paper in Table 11.3 . The TABLE 11.3 . COMPARISON OF OBSERVED AND CALCULATED VALUES OF THE ELECTRICAL CONDUCTIVITY AT 0 ° C ...
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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