Introduction to Solid State Physicsproblems after each chapter |
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Page 104
We consider the forces acting on an element of length Ax . At one end of the element the strain is e ( x ) , and at the other end it is e ( x + A.x ) = e ( x ) + ( de / 8x ) Ax = e ( x ) + ( a'u / ox ? ) At , and so the resultant force ...
We consider the forces acting on an element of length Ax . At one end of the element the strain is e ( x ) , and at the other end it is e ( x + A.x ) = e ( x ) + ( de / 8x ) Ax = e ( x ) + ( a'u / ox ? ) At , and so the resultant force ...
Page 553
In order to compute DB and Dp for grain - boundary diffusion , they consider an incoherent grain boundary to be a thin slab of low - resistance material , SA thick , of diffusivity Ds . They similarly consider each dislocation in a low ...
In order to compute DB and Dp for grain - boundary diffusion , they consider an incoherent grain boundary to be a thin slab of low - resistance material , SA thick , of diffusivity Ds . They similarly consider each dislocation in a low ...
Page 576
Onsager has carried out an approximate treatment of the latter situation by considering a very small spherical cavity , just large enough to contain one molecule . If we consider this cavity real , we may ask what is the value of the ...
Onsager has carried out an approximate treatment of the latter situation by considering a very small spherical cavity , just large enough to contain one molecule . If we consider this cavity real , we may ask what is the value of 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