Introduction to Solid State Physicsproblems after each chapter |
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Page 26
CHARACTERISTICS OF CUBIC LATTICES Simple Body - Centered Face -
Centered Unit cell volume a3 a3 Lattice points per cell Lattice points per unit
volume 1 / a3 Nearest neighbor distance 340 / 2 a / 242 Number of nearest
neighbors ...
CHARACTERISTICS OF CUBIC LATTICES Simple Body - Centered Face -
Centered Unit cell volume a3 a3 Lattice points per cell Lattice points per unit
volume 1 / a3 Nearest neighbor distance 340 / 2 a / 242 Number of nearest
neighbors ...
Page 67
That is , each carbon atom will be at the center of the tetrahedron formed by the
nearest neighbor atoms . ... tetrahedral bond allows only four nearest neighbors ,
while a closest - packed structure would require twelve nearest neighbor atoms .
That is , each carbon atom will be at the center of the tetrahedron formed by the
nearest neighbor atoms . ... tetrahedral bond allows only four nearest neighbors ,
while a closest - packed structure would require twelve nearest neighbor atoms .
Page 97
If a is the nearest neighbor distance , we may write for the energy density for a
homogeneous pure strain U = Naa " ( exx ... We note that with only nearest
neighbor forces on the central force assumption ( B = 0 ) the simple cubic lattice
does not ...
If a is the nearest neighbor distance , we may write for the energy density for a
homogeneous pure strain U = Naa " ( exx ... We note that with only nearest
neighbor forces on the central force assumption ( B = 0 ) the simple cubic lattice
does not ...
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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 neighbor 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