Introduction to Solid State PhysicsProblems after each chapter. |
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Page 121
... Heat capacity of metallic silver as a function of temperature . The heat capacity at constant pressure , Cp , is the quantity measured , but for solids below room temperature the difference between C , and C , is small and usually may ...
... Heat capacity of metallic silver as a function of temperature . The heat capacity at constant pressure , Cp , is the quantity measured , but for solids below room temperature the difference between C , and C , is small and usually may ...
Page 135
... heat capacity , where N is the number of conduction electrons per unit volume . That is , one would be led to expect ( for T >> ) a total heat capacity of 3R per mole for insulators and ( 3 + ) R = 9R / 2 per mole for metals . In fact the ...
... heat capacity , where N is the number of conduction electrons per unit volume . That is , one would be led to expect ( for T >> ) a total heat capacity of 3R per mole for insulators and ( 3 + ) R = 9R / 2 per mole for metals . In fact the ...
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 ...
... 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 ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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absorption acceptors alkali alloys approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point levels low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero