Introduction to Solid State Physicsproblems after each chapter |
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Page 299
We now consider in detail the motion of a hole in an applied electric field . We treat the one - dimensional example illustrated by Fig . 11.15 . Initially the band is filled except for the single vacant state F at the top of the band .
We now consider in detail the motion of a hole in an applied electric field . We treat the one - dimensional example illustrated by Fig . 11.15 . Initially the band is filled except for the single vacant state F at the top of the band .
Page 553
Motion of the boundary took place by cooperative motion of the dislocations in the array , each dislocation moving an equal distance in its own slip plane . Opposite top and bottom intersections at the boundary with the surface moved ...
Motion of the boundary took place by cooperative motion of the dislocations in the array , each dislocation moving an equal distance in its own slip plane . Opposite top and bottom intersections at the boundary with the surface moved ...
Page 559
There appear to be four important ways of increasing the yield strength of an alloy so that it will withstand shear stresses as high as 10 - G . They are mechanical blocking of dislocation motion , pinning of dislocations by solute ...
There appear to be four important ways of increasing the yield strength of an alloy so that it will withstand shear stresses as high as 10 - G . They are mechanical blocking of dislocation motion , pinning of dislocations by solute ...
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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