Physical Properties of Crystals |
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Page 24
... orientation . We need three numbers to specify the lengths of the quadric axes , that is , the shape of the quadric , and one more to decide the orientation ( say the angle through which it has to be turned from some arbitrary position ) ...
... orientation . We need three numbers to specify the lengths of the quadric axes , that is , the shape of the quadric , and one more to decide the orientation ( say the angle through which it has to be turned from some arbitrary position ) ...
Page 62
... orientation , because in a given applied field the same volume of an isotropic crystal placed in different orientations or made into different shapes will experience different couples . The size of the couple may be estimated as follows ...
... orientation , because in a given applied field the same volume of an isotropic crystal placed in different orientations or made into different shapes will experience different couples . The size of the couple may be estimated as follows ...
Page 104
... orientation , with the position of the point . = Y + Yar - FIG . 6.11 . Illustrating that a simple shear ( left - hand diagram ) equals a pure shear ( centre diagram ) plus a rotation ( right- hand diagram ) . 4. Strain and crystal ...
... orientation , with the position of the point . = Y + Yar - FIG . 6.11 . Illustrating that a simple shear ( left - hand diagram ) equals a pure shear ( centre diagram ) plus a rotation ( right- hand diagram ) . 4. Strain and crystal ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 11 |
EQUILIBRIUM PROPERTIES | 45 |
PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY | 53 |
20 other sections not shown
Common terms and phrases
angle anisotropic applied biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined deformation denoted diad axis dielectric dijk displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ 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 pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress suffixes symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal wave surface x₁ Young's Modulus zero ат