Introduction to Solid State Physics |
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Page 53
If then a cubic crystal were elastically isotropic and the Cauchy relation satisfied ,
the velocity of the transverse waves would be equal to $ ? ? the velocity of the
longitudinal waves . The conditions for the validity of the Cauchy relations are : 1 .
If then a cubic crystal were elastically isotropic and the Cauchy relation satisfied ,
the velocity of the transverse waves would be equal to $ ? ? the velocity of the
longitudinal waves . The conditions for the validity of the Cauchy relations are : 1 .
Page 309
EINSTEIN RELATION The ionic conductivity , mobility , and self - diffusion
coefficients are closely related . We recall that the mobility is defined as the drift
velocity per unit electric field . If only one ion type , for example the interstitial
cations , is ...
EINSTEIN RELATION The ionic conductivity , mobility , and self - diffusion
coefficients are closely related . We recall that the mobility is defined as the drift
velocity per unit electric field . If only one ion type , for example the interstitial
cations , is ...
Page 309
EINSTEIN RELATION The ionic conductivity , mobility , and self - diffusion
coefficients are closely related . We recall that the mobility is defined as the drift
velocity per unit electric field . If only one ion type , for example the interstitial
cations , is ...
EINSTEIN RELATION The ionic conductivity , mobility , and self - diffusion
coefficients are closely related . We recall that the mobility is defined as the drift
velocity per unit electric field . If only one ion type , for example the interstitial
cations , is ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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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