Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 40
... length . This evidently reverses quantities which are polar vectors , but leaves unchanged quantities which are axial vectors . On the other hand , reflection of each symbol in a plane parallel to its length has the opposite effect . 13 ...
... length . This evidently reverses quantities which are polar vectors , but leaves unchanged quantities which are axial vectors . On the other hand , reflection of each symbol in a plane parallel to its length has the opposite effect . 13 ...
Page 49
... length and direction ( Fig . 2.2 a ) . An axial vector can be visualized as a length with a definite orientation and with a definite sense of rotation attached to it ( Fig . 2.2 b ) . Principal axes of a tensor ( § 3 ) . The principal ...
... length and direction ( Fig . 2.2 a ) . An axial vector can be visualized as a length with a definite orientation and with a definite sense of rotation attached to it ( Fig . 2.2 b ) . Principal axes of a tensor ( § 3 ) . The principal ...
Page 100
... length , or the stretch , of a line drawn originally in that direction . Fig . 6.8a makes this clear . The vector 1 represents a line of unit length in the unstrained body . On straining , it changes both in length and direction . The ...
... length , or the stretch , of a line drawn originally in that direction . Fig . 6.8a makes this clear . The vector 1 represents a line of unit length in the unstrained body . On straining , it changes both in length and direction . The ...
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