Introduction to Solid State Physicsproblems after each chapter |
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Page 34
The indices of a direction in a crystal are expressed as the set of the smallest integers which have the same ratios as the components of a vector in the desired direction referred to the axis vectors . The integers are written between ...
The indices of a direction in a crystal are expressed as the set of the smallest integers which have the same ratios as the components of a vector in the desired direction referred to the axis vectors . The integers are written between ...
Page 102
A cubic crystal is subject to tension in the ( 100 ) direction . Find expressions for Young's modulus and Poisson's ratio in terms of the elastic compliances or stiffnesses . 4.5 . Show that the velocity of propagation of a shear wave ...
A cubic crystal is subject to tension in the ( 100 ) direction . Find expressions for Young's modulus and Poisson's ratio in terms of the elastic compliances or stiffnesses . 4.5 . Show that the velocity of propagation of a shear wave ...
Page 428
The excess energy required in the hard direction is the anisotropy energy . ... The direction of the hexagonal axis is the direction of easy magnetization ( at room temperature ) , while all directions in the basal plane , normal to the ...
The excess energy required in the hard direction is the anisotropy energy . ... The direction of the hexagonal axis is the direction of easy magnetization ( at room temperature ) , while all directions in the basal plane , normal to the ...
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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