Introduction to Solid State Physics |
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Page 177
The essential difference between material for permanent magnets and material
for transformer cores lies in the coercive force , which may range from the value
of 600 oersteds in a loudspeaker magnet ( Alnico V ) and 20 , 000 in a special
high ...
The essential difference between material for permanent magnets and material
for transformer cores lies in the coercive force , which may range from the value
of 600 oersteds in a loudspeaker magnet ( Alnico V ) and 20 , 000 in a special
high ...
Page 301
Make a cut along any simple surface bounded by the line . Displace the material
on one side of this surface by d relative to the other side ; d is a fixed vector called
the Burgers vector . In regions where d is not parallel to the surface this relative ...
Make a cut along any simple surface bounded by the line . Displace the material
on one side of this surface by d relative to the other side ; d is a fixed vector called
the Burgers vector . In regions where d is not parallel to the surface this relative ...
Page 310
The material is soft in this condition . When the radius of curvature is comparable
with the particle spacing , each wiggle of the dislocation line must be carried
separately through the stress field of each precipitate particle . In this case the ...
The material is soft in this condition . When the radius of curvature is comparable
with the particle spacing , each wiggle of the dislocation line must be carried
separately through the stress field of each precipitate particle . In this case the ...
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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