Introduction to Solid State Physics |
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Page 51
A shear wave propagates along a cube axis with velocity ( C44 / p ) " , while a
shear wave with particle motion along a 170 ... ELASTIC WAVES IN CUBIC
CRYSTALS By considering the forces acting on an element of volume in the
crystal we ...
A shear wave propagates along a cube axis with velocity ( C44 / p ) " , while a
shear wave with particle motion along a 170 ... ELASTIC WAVES IN CUBIC
CRYSTALS By considering the forces acting on an element of volume in the
crystal we ...
Page 52
There is also a solution given by a shear wave moving in the z direction with
particle motion in the x direction . In general there are three types of wave motion
for a given direction of propagation in the crystal , but only for a few special ...
There is also a solution given by a shear wave moving in the z direction with
particle motion in the x direction . In general there are three types of wave motion
for a given direction of propagation in the crystal , but only for a few special ...
Page 264
where B is the amplitude ; 10 we suppose that r is sufficiently far from ro so that in
the vicinity of r the scattered wave may ' be treated as a plane wave in the
direction k . The amplitude B will be proportional to the strength of the incident
wave at ...
where B is the amplitude ; 10 we suppose that r is sufficiently far from ro so that in
the vicinity of r the scattered wave may ' be treated as a plane wave in the
direction k . The amplitude B will be proportional to the strength of the incident
wave at ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero