Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 239
John Frederick Nye. principal axis equal to no . The other principal axis will be intermediate in length between n 。 and n ̧ ( Fig . 13.2 ) . We know that two waves are Optic axis Optic axis a b FIG . 13.4 . The wave surface for a ...
John Frederick Nye. principal axis equal to no . The other principal axis will be intermediate in length between n 。 and n ̧ ( Fig . 13.2 ) . We know that two waves are Optic axis Optic axis a b FIG . 13.4 . The wave surface for a ...
Page 263
... optic axis , because in these cases one can study optical activity free from the effects of ordinary birefringence . We must now ask : if this effect can occur when light is transmitted along an optic axis in bire- fringent crystals ...
... optic axis , because in these cases one can study optical activity free from the effects of ordinary birefringence . We must now ask : if this effect can occur when light is transmitted along an optic axis in bire- fringent crystals ...
Page 273
John Frederick Nye. along the optic axes , and so manifestations of optical activity must be sought in other ... axis . If they are so related , the rotations along each must be the same ; if they are not so related , the rotations along ...
John Frederick Nye. along the optic axes , and so manifestations of optical activity must be sought in other ... axis . If they are so related , the rotations along each must be the same ; if they are not so related , the rotations along ...
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