Introduction to Solid State Physicsproblems after each chapter |
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Page 547
Screw dislocations of like sign repel 6 each other to infinity , and those of opposite sign attract each other until they annihilate , 6 1 1 LOW - ANGLE GRAIN BOUNDARIES D = - 8 Burgers ? suggested that low - angle grain boundaries in ...
Screw dislocations of like sign repel 6 each other to infinity , and those of opposite sign attract each other until they annihilate , 6 1 1 LOW - ANGLE GRAIN BOUNDARIES D = - 8 Burgers ? suggested that low - angle grain boundaries in ...
Page 550
If two portions of a crystal are rotated through a small angle about an axis perpendicular to the resulting grain boundary , instead of about Fig . 19.14 . Dislocation etch pits in low - angle boundary on ( 100 ) face of germanium ...
If two portions of a crystal are rotated through a small angle about an axis perpendicular to the resulting grain boundary , instead of about Fig . 19.14 . Dislocation etch pits in low - angle boundary on ( 100 ) face of germanium ...
Page 553
One side of the crystal was clamped , and a force was applied at a point on the opposite side of the boundary . Motion of the boundary took place by cooperative motion of the dislocations in the array , each dislocation moving an equal ...
One side of the crystal was clamped , and a force was applied at a point on the opposite side of the boundary . Motion of the boundary took place by cooperative motion of the dislocations in the array , each dislocation moving an equal ...
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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