Introduction to Solid State Physicsproblems after each chapter |
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Page 150
Berman24 has measured the thermal conductivity of three alloys ( German silver ,
stainless steel , and constantan ) between 2° and 90°K and found electron and
phonon contributions of equal orders of magnitude . The total thermal resistivity ...
Berman24 has measured the thermal conductivity of three alloys ( German silver ,
stainless steel , and constantan ) between 2° and 90°K and found electron and
phonon contributions of equal orders of magnitude . The total thermal resistivity ...
Page 239
Experimental points involving resistivity measurements of Cu and Ag films at
room temperature , shown with curves calculated from theory to obtain
approximate values of mean free paths . Here é is the resistivity in the film ; p is
the bulk ...
Experimental points involving resistivity measurements of Cu and Ag films at
room temperature , shown with curves calculated from theory to obtain
approximate values of mean free paths . Here é is the resistivity in the film ; p is
the bulk ...
Page 270
Yet the distinction between the resistivity values of conductors , superconductivity
apart , and insulators is striking : the resistivity of a pure metal at low
temperatures may be of the order of 10 - 8 ohm - cm , and the resistivity of a good
insulator ...
Yet the distinction between the resistivity values of conductors , superconductivity
apart , and insulators is striking : the resistivity of a pure metal at low
temperatures may be of the order of 10 - 8 ohm - cm , and the resistivity of a good
insulator ...
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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 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