Introduction to Solid State Physicsproblems after each chapter |
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Page 121
theory predicts the lattice contribution to the molar heat capacity at constant
volume al'a ( 6.10 ) Co COM ar V of a solid should be , for a mole of atoms , ( 6.11
) C , = 3R = 6 calories / deg mole . This value , which is known as the Dulong and
...
theory predicts the lattice contribution to the molar heat capacity at constant
volume al'a ( 6.10 ) Co COM ar V of a solid should be , for a mole of atoms , ( 6.11
) C , = 3R = 6 calories / deg mole . This value , which is known as the Dulong and
...
Page 135
If the conduction electrons behaved as free classical particles , they would make
a contribution l'el = Nk to the heat capacity , where N is the number of conduction
electrons per unit volume . That is , one would be led to expect ( for T >> O ) a ...
If the conduction electrons behaved as free classical particles , they would make
a contribution l'el = Nk to the heat capacity , where N is the number of conduction
electrons per unit volume . That is , one would be led to expect ( for T >> O ) a ...
Page 136
Heat capacity of metallic silver . ( According to Corak , Garfunkel , Satterthwaite ,
and Wexler . ) the temperature dependence of the conduction electron heat
capacity is actually linear in T for most metals ; however , the coefficient y may
have ...
Heat capacity of metallic silver . ( According to Corak , Garfunkel , Satterthwaite ,
and Wexler . ) the temperature dependence of the conduction electron heat
capacity is actually linear in T for most metals ; however , the coefficient y may
have ...
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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 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