Introduction to Solid State Physicsproblems after each chapter |
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Page 105
If both bonds increase in length , the two forces on atom n will be oppositely directed . Here is the force constant . Looked at on a macroscopic scale , the line has a linear density p = M / a , as there are 1 / a atoms per a M unit ...
If both bonds increase in length , the two forces on atom n will be oppositely directed . Here is the force constant . Looked at on a macroscopic scale , the line has a linear density p = M / a , as there are 1 / a atoms per a M unit ...
Page 480
We note that the production of Schottky defects lowers the density of the crystal because the net result of their production is an increase in the volume of the + -Frenkel Se + + Schottky Fig . 17.2 . Schottky and Frenkel defects in an ...
We note that the production of Schottky defects lowers the density of the crystal because the net result of their production is an increase in the volume of the + -Frenkel Se + + Schottky Fig . 17.2 . Schottky and Frenkel defects in an ...
Page 557
No dislocations can be present in thermal equilibrium , because their energy is much too great in comparison with the increase in entropy that they produce . They must therefore be introduced in a non - equilibrium manner during the ...
No dislocations can be present in thermal equilibrium , because their energy is much too great in comparison with the increase in entropy that they produce . They must therefore be introduced in a non - equilibrium manner during the ...
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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