Introduction to Solid State Physicsproblems after each chapter |
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Page 135
In fact the heat capacity of metals at high temperatures usually is not particularly
different from that of insulators . ... For normal metals the definition of a low
temperature for the present purpose is by comparison with a temperature of the
order ...
In fact the heat capacity of metals at high temperatures usually is not particularly
different from that of insulators . ... For normal metals the definition of a low
temperature for the present purpose is by comparison with a temperature of the
order ...
Page 242
involves neither N , m , or T . A more detailed study of the quantum theory of
transport processes in metals shows that the Lorenz number is expected to be
independent of temperature only above the Debye temperature , as the
differences ...
involves neither N , m , or T . A more detailed study of the quantum theory of
transport processes in metals shows that the Lorenz number is expected to be
independent of temperature only above the Debye temperature , as the
differences ...
Page 301
Theoretical ( Grüneisen ) temperature variation of electrical resistance , and
experimental values for various metals . ( After Bardeen . ) first quantum
calculations were made by Bloch . In the high temperature region the calculated
conductivity ...
Theoretical ( Grüneisen ) temperature variation of electrical resistance , and
experimental values for various metals . ( After Bardeen . ) first quantum
calculations were made by Bloch . In the high temperature region the calculated
conductivity ...
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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