Introduction to Solid State Physics |
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Page 46
Thus the stress component X . represents a force applied in the x direction to a
unit area of a plane whose normal lies in ... Demonstration that number of
independent stress components Yo = Xy in order that the is reduced to six by
applying to ...
Thus the stress component X . represents a force applied in the x direction to a
unit area of a plane whose normal lies in ... Demonstration that number of
independent stress components Yo = Xy in order that the is reduced to six by
applying to ...
Page 89
Dielectric Properties In this chapter we discuss first the relationship between the
applied electric field and the local electric field acting on an atom . The interaction
of the local field with the atom determines the polarization , yet the local field ...
Dielectric Properties In this chapter we discuss first the relationship between the
applied electric field and the local electric field acting on an atom . The interaction
of the local field with the atom determines the polarization , yet the local field ...
Page 91
principal axes parallel to the applied field , the polarization will be parallel to the
applied field , as will the depolarization field E1 , which it is found may be
calculated from the polarization P by a relation of the form ( 6 . 3 ) E1 = - NP .
principal axes parallel to the applied field , the polarization will be parallel to the
applied field , as will the depolarization field E1 , which it is found may be
calculated from the polarization P by a relation of the form ( 6 . 3 ) E1 = - NP .
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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