Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 19
... give P1 = Sij qj . Pi ( 29 ) If [ S ] is now referred to its principal axes , equations ( 29 ) written out in full ... gives j1 and j2 , which then compound to give j . The fact that j is not parallel to E is a direct = consequence of ...
... give P1 = Sij qj . Pi ( 29 ) If [ S ] is now referred to its principal axes , equations ( 29 ) written out in full ... gives j1 and j2 , which then compound to give j . The fact that j is not parallel to E is a direct = consequence of ...
Page 45
... gives a visual picture of the way S11 , S22 and S12 change as the axes of reference are rotated . As Ox1 in Fig . 2.4a rotates from Ox1 to Ox2 , 9 changes from 0 to π , and R moves round the upper half of the circle in Fig . 2.46 from Q ...
... gives a visual picture of the way S11 , S22 and S12 change as the axes of reference are rotated . As Ox1 in Fig . 2.4a rotates from Ox1 to Ox2 , 9 changes from 0 to π , and R moves round the upper half of the circle in Fig . 2.46 from Q ...
Page 257
... gives rise to second derivatives of strain with respect to the field . If the field is reversed in direction , all ... give finite values 5788 S § 3 257 SECOND - ORDER EFFECTS.
... gives rise to second derivatives of strain with respect to the field . If the field is reversed in direction , all ... give finite values 5788 S § 3 257 SECOND - ORDER EFFECTS.
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
EQUILIBRIUM PROPERTIES | 51 |
ELECTRIC POLARIZATION | 68 |
18 other sections not shown
Common terms and phrases
angle anisotropic applied axial vector centre of symmetry Chapter coefficients conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals defined denoted diad axis dielectric dijk direction cosines dummy suffix elastic electric field ellipsoid equation example force given grad H₁ H₂ heat flow Hence hexagonal homogeneous indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic effect piezoelectric effect plane plate polarization principal axes produced pyroelectric pyroelectric effect quantities radius vector referred refractive index relation representation quadric represented right-handed rotation S₁ scalar second-rank tensor set of axes shear strain stress suffix notation surface susceptibility symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values x₁ Young's Modulus zero