Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 69
... dielectric constant . In an anisotropic substance we have , in place of ( 2 ) , P1 = Ko Xij Ej , where X is the dielectric susceptibility tensor ; instead of ( 3 ) we have Xij Kij D1 = K1j Ej , Di ( 4 ) ( 5 ) ( 6 ) where is the ...
... dielectric constant . In an anisotropic substance we have , in place of ( 2 ) , P1 = Ko Xij Ej , where X is the dielectric susceptibility tensor ; instead of ( 3 ) we have Xij Kij D1 = K1j Ej , Di ( 4 ) ( 5 ) ( 6 ) where is the ...
Page 71
... dielectric anomalies ' , caused by the fact that the dielectrics are not perfectly insulating . Consider the following example . A flat slab of dielectric is placed between two parallel condenser plates and separated from them by narrow ...
... dielectric anomalies ' , caused by the fact that the dielectrics are not perfectly insulating . Consider the following example . A flat slab of dielectric is placed between two parallel condenser plates and separated from them by narrow ...
Page 72
... dielectric permittivity of vacuum capacity with dielectric capacity without dielectric = dielectric constant . But , if the dielectric is an anisotropic crystal in an arbitrary orientation , the question arises as to what ' permittivity ...
... dielectric permittivity of vacuum capacity with dielectric capacity without dielectric = dielectric constant . But , if the dielectric is an anisotropic crystal in an arbitrary orientation , the question arises as to what ' permittivity ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
3 | 29 |
EQUILIBRIUM PROPERTIES | 51 |
23 other sections not shown
Common terms and phrases
angle anisotropic applied axial B₁ biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined denoted diad axis dielectric dijk direction cosines displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ H₂ heat flow Hence hexagonal indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optic axis optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic photoelastic effect piezoelectric effect plane plate polarization positive principal axes produced pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal x₁ zero әт