Introduction to Solid State Physicsproblems after each chapter |
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Page 88
There are nine stress components : X ~ , Xy , X2 , Y . , Yy , Y , ZX , Zy , Zz . The
capital letter indicates the direction of the force , and the subscript indicates the
normal to the plane to which the force is applied . Thus the stress component X ...
There are nine stress components : X ~ , Xy , X2 , Y . , Yy , Y , ZX , Zy , Zz . The
capital letter indicates the direction of the force , and the subscript indicates the
normal to the plane to which the force is applied . Thus the stress component X ...
Page 167
of ions of opposite sign when an electric field is applied , and also from the
deformation of the electronic shells of the ions as a result of the relative motion of
the ions . We consider the situation in a sodium chloride crystal when a uniform ...
of ions of opposite sign when an electric field is applied , and also from the
deformation of the electronic shells of the ions as a result of the relative motion of
the ions . We consider the situation in a sodium chloride crystal when a uniform ...
Page 180
14 ) applied to the first Bohr orbit of the hydrogen atom gives a = an " , where ay
is the Bohr radius . ( b ) Consider a semiclassical model of the ground state of the
hydrogen atom in an electric field normal to the plane of the orbit , and show that
...
14 ) applied to the first Bohr orbit of the hydrogen atom gives a = an " , where ay
is the Bohr radius . ( b ) Consider a semiclassical model of the ground state of the
hydrogen atom in an electric field normal to the plane of the orbit , and show that
...
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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