Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 236
... indicatrix . B X3 -X2 FIG . 13.1 . The indicatrix construction giving the two refractive indices and the vibration directions of D for the two plane polarized waves associated with a given wave normal . If x1 , x2 , x3 are the principal ...
... indicatrix . B X3 -X2 FIG . 13.1 . The indicatrix construction giving the two refractive indices and the vibration directions of D for the two plane polarized waves associated with a given wave normal . If x1 , x2 , x3 are the principal ...
Page 237
... indicatrix are subject to the same limitations as the representation quadric for a second - rank tensor pro- perty ( Ch . I , § 5.1 ) . It follows that the indicatrix for a cubic crystal is a sphere and , since all central sections are ...
... indicatrix are subject to the same limitations as the representation quadric for a second - rank tensor pro- perty ( Ch . I , § 5.1 ) . It follows that the indicatrix for a cubic crystal is a sphere and , since all central sections are ...
Page 238
... indicatrix , and the two primary optic axes OP1 , OP , for a biaxial crystal . Both circular sections contain the principal axis of the indicatrix that is intermediate in length between the other two . Their radius is therefore equal to ...
... indicatrix , and the two primary optic axes OP1 , OP , for a biaxial crystal . Both circular sections contain the principal axis of the indicatrix that is intermediate in length between the other two . Their radius is therefore equal to ...
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