Introduction to Solid State Physicsproblems after each chapter |
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234 10 · FREE ELECTRON MODEL OF METALS Electrical conductivity and Ohm's law . Wiedemann - Franz ratio . Heat capacity of conduction electrons . Paramagnetic susceptibility of conduction electrons . Quantum theory of free particles in a ...
234 10 · FREE ELECTRON MODEL OF METALS Electrical conductivity and Ohm's law . Wiedemann - Franz ratio . Heat capacity of conduction electrons . Paramagnetic susceptibility of conduction electrons . Quantum theory of free particles in a ...
Page 234
10 Free Electron Model of Metals It is possible to understand a number of important physical properties of some metals , in particular the simple monovalent metals , in terms of the free electron model . According to this model the ...
10 Free Electron Model of Metals It is possible to understand a number of important physical properties of some metals , in particular the simple monovalent metals , in terms of the free electron model . According to this model the ...
Page 346
W. Hume - Rothery , Structure of metals and alloys , Institute of Metals , London , 1947 . W. Hume - Rothery and B. R. Coles , “ Transition metals and their alloys , ” Advances in Physics 3 , 149–243 ( 1954 ) .
W. Hume - Rothery , Structure of metals and alloys , Institute of Metals , London , 1947 . W. Hume - Rothery and B. R. Coles , “ Transition metals and their alloys , ” Advances in Physics 3 , 149–243 ( 1954 ) .
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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