Introduction to Solid State Physicsproblems after each chapter |
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Page 304
The extension of the theory to the region T « is indicated in Appendix K. It has been found by Grüneisen 17 that the observed temperature dependence of the resistivity is described quite well at all temperatures by the semi - empirical ...
The extension of the theory to the region T « is indicated in Appendix K. It has been found by Grüneisen 17 that the observed temperature dependence of the resistivity is described quite well at all temperatures by the semi - empirical ...
Page 305
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 ...
Page 562
Actually Volmer and Schultze observed growth of iodine crystals at vapor supersaturations down to less than 1 percent , where the ... This has been referred to as an all - time record for disagreement between observation and theory .
Actually Volmer and Schultze observed growth of iodine crystals at vapor supersaturations down to less than 1 percent , where the ... This has been referred to as an all - time record for disagreement between observation and theory .
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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