Introduction to Solid State Physicsproblems after each chapter |
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Page 326
ELECTRON / Atom Ratios OF ELECTRON COMPOUNDS Minimum a - phase B -
phase r - phase e - phase Alloy Boundary Boundary Boundaries Boundaries Cu -
Zn 1.38 1.48 1.58-1.66 1.78-1.87 Cu - Al 1.41 1.48 1.63–1.77 Cu - Ga 1.41 Cu ...
ELECTRON / Atom Ratios OF ELECTRON COMPOUNDS Minimum a - phase B -
phase r - phase e - phase Alloy Boundary Boundary Boundaries Boundaries Cu -
Zn 1.38 1.48 1.58-1.66 1.78-1.87 Cu - Al 1.41 1.48 1.63–1.77 Cu - Ga 1.41 Cu ...
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 ; the
angle of the ...
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 ; the
angle of the ...
Page 553
19.16 . The specimen consisted of a bicrystal of zinc containing a 2 ° tilt
boundThe dislocations are about thirty atomic planes apart . One side of the
crystal was clamped , and a force was applied at a point on the opposite side of
the boundary .
19.16 . The specimen consisted of a bicrystal of zinc containing a 2 ° tilt
boundThe dislocations are about thirty atomic planes apart . One side of the
crystal was clamped , and a force was applied at a point on the opposite side of
the boundary .
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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 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