Introduction to Solid State Physicsproblems after each chapter |
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Page 88
Thus the stress component X , represents a force applied in the x direcY , tion to a unit area of a plane whose normal lies in the x direction ; the stress component x , represents a force applied in the x direction to a unit area ...
Thus the stress component X , represents a force applied in the x direcY , tion to a unit area of a plane whose normal lies in the x direction ; the stress component x , represents a force applied in the x direction to a unit area ...
Page 173
tion is neglected , the Onsager model gives ( 7.32 ) 1 [ 1 + 3x + 3 ( 1 + ģx + x ? ) ? ] , x = 4nNp2 / 3kT . It is easily seen that this expression , which is derived in Appendix C , does not give a critical point .
tion is neglected , the Onsager model gives ( 7.32 ) 1 [ 1 + 3x + 3 ( 1 + ģx + x ? ) ? ] , x = 4nNp2 / 3kT . It is easily seen that this expression , which is derived in Appendix C , does not give a critical point .
Page 564
The result is a permanent step extending across a por tion of the crystal face and anchored at the boundary of the cut . Molecules depositing on the surface from a vapor would lodge against the step , causing it to advance .
The result is a permanent step extending across a por tion of the crystal face and anchored at the boundary of the cut . Molecules depositing on the surface from a vapor would lodge against the step , causing it to advance .
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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