Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 83
... cube upon the material inside the cube . The force transmitted across each face may be resolved into three components . Consider first the three faces which are towards the three positive ends of the axes ( those shown in Fig . 5.1 ) ...
... cube upon the material inside the cube . The force transmitted across each face may be resolved into three components . Consider first the three faces which are towards the three positive ends of the axes ( those shown in Fig . 5.1 ) ...
Page 136
... cube , and suppose it is subjected to a small homogeneous strain with components . Now let the strain components all be changed to e + de . We prove that the work done by the stress components σ acting on the cube faces is dW = ode ...
... cube , and suppose it is subjected to a small homogeneous strain with components . Now let the strain components all be changed to e + de . We prove that the work done by the stress components σ acting on the cube faces is dW = ode ...
Page 254
... cube axis and measuring the resulting birefringence at right angles to the stress axis , the values of ( 11-12 ) and ( 711-713 ) can be found . Such measurements of bire- fringence are comparatively easy to make . It may be shown ...
... cube axis and measuring the resulting birefringence at right angles to the stress axis , the values of ( 11-12 ) and ( 711-713 ) can be found . Such measurements of bire- fringence are comparatively easy to make . It may be shown ...
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