Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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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 + λέγ L - 5 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 + λέγ L - 5 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 ...
Page 123
... orientation ) m 1x2 ( standard orientation ) ( 18 ) MONOCLINIC Class 2 Class 2 2 || x ( 8 ) ( 8 ) Class m Class m m1xs 9 ORTHORHOMBIC Class 222 Class mm2 Class 4 ( 3 ) ( 10 ) ( 5 ) :) TETRAGONAL ( 4 ) Class 7 × ( X ) . ( 4 ) f Class 422 ...
... orientation ) m 1x2 ( standard orientation ) ( 18 ) MONOCLINIC Class 2 Class 2 2 || x ( 8 ) ( 8 ) Class m Class m m1xs 9 ORTHORHOMBIC Class 222 Class mm2 Class 4 ( 3 ) ( 10 ) ( 5 ) :) TETRAGONAL ( 4 ) Class 7 × ( X ) . ( 4 ) f Class 422 ...
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