Introduction to Solid State Physicsproblems after each chapter |
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Page 88
STRESS COMPONENTS a The force acting on a unit area in the solid is defined as the stress . There are nine stress components : Xă , Xy , X2 , Y. , Yu , Y. , Z2 , Zy , Zz . The capital letter indicates the direction of the force ...
STRESS COMPONENTS a The force acting on a unit area in the solid is defined as the stress . There are nine stress components : Xă , Xy , X2 , Y. , Yu , Y. , Z2 , Zy , Zz . The capital letter indicates the direction of the force ...
Page 105
to deal with nearest neighbor interactions alone , the force Fn acting on the nth atom may be written ( 5.5 ) Fn B ( unt1 – un ) – B ( Un – Un - 1 ) , the first term in parentheses on the right being the increase in length of the bond ...
to deal with nearest neighbor interactions alone , the force Fn acting on the nth atom may be written ( 5.5 ) Fn B ( unt1 – un ) – B ( Un – Un - 1 ) , the first term in parentheses on the right being the increase in length of the bond ...
Page 422
COERCIVE FORCE AND HYSTERESIS The coercive force is perhaps the most sensitive property of ferromagnetic materials which is subject to our control , and it is one of the most important criteria in the selection of ferromagnetic ...
COERCIVE FORCE AND HYSTERESIS The coercive force is perhaps the most sensitive property of ferromagnetic materials which is subject to our control , and it is one of the most important criteria in the selection of ferromagnetic ...
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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