Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page xiii
... produced by a temperature gradient ( thermal con- ductivity ) ; the polarization produced in a dielectric by an electric field ( dielectric susceptibility ) ; the polarization of a crystal that may be produced by mechanical stress ...
... produced by a temperature gradient ( thermal con- ductivity ) ; the polarization produced in a dielectric by an electric field ( dielectric susceptibility ) ; the polarization of a crystal that may be produced by mechanical stress ...
Page 125
... produce a polarization along x1 : axes Ox1 , 0x2 , 0x3 . P1 = d12 , P2 = 0 , P = 0 -d1102 , ( second column of the matrix ) . A given polarization along the diad axis x1 may therefore be produced either by a tensile stress along x1 or ...
... produce a polarization along x1 : axes Ox1 , 0x2 , 0x3 . P1 = d12 , P2 = 0 , P = 0 -d1102 , ( second column of the matrix ) . A given polarization along the diad axis x1 may therefore be produced either by a tensile stress along x1 or ...
Page 171
... produced by a stress . The two horizontal lines at the bottom show that entropy ( heat ) is produced by strain as heat of deformation , and that if the temperature of a crystal is changed without change of shape being allowed to take ...
... produced by a stress . The two horizontal lines at the bottom show that entropy ( heat ) is produced by strain as heat of deformation , and that if the temperature of a crystal is changed without change of shape being allowed to take ...
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