Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 5
... applied along Ox1 . meaning . For instance , if the field is applied along x1 † ( Fig . 1.2 ) , E = [ E1 , 0 , 0 ] , and equations ( 3 ) become ji = 011 E1 j2 j2 = 021 E1 . j3 = 031 E1 Thus , there are now components of j not only along ...
... applied along Ox1 . meaning . For instance , if the field is applied along x1 † ( Fig . 1.2 ) , E = [ E1 , 0 , 0 ] , and equations ( 3 ) become ji = 011 E1 j2 j2 = 021 E1 . j3 = 031 E1 Thus , there are now components of j not only along ...
Page 111
... applied in turn along Ox , and Ox , physical meanings may be attached to the other dijk coefficients in which j = k . Suppose now that a pure shear stress σ12 is applied . We have to remember that , if body - torques are ignored ( p ...
... applied in turn along Ox , and Ox , physical meanings may be attached to the other dijk coefficients in which j = k . Suppose now that a pure shear stress σ12 is applied . We have to remember that , if body - torques are ignored ( p ...
Page 132
... applied parallel to one set of edges , it will not only stretch in the direction of the tension but it may also ... applied , remembering that without body - torquest 12 cannot be applied without σ21 , we should have = € 11 81112 12 + ...
... applied parallel to one set of edges , it will not only stretch in the direction of the tension but it may also ... applied , remembering that without body - torquest 12 cannot be applied without σ21 , we should have = € 11 81112 12 + ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
3 | 29 |
EQUILIBRIUM PROPERTIES | 51 |
23 other sections not shown
Common terms and phrases
angle anisotropic applied axial B₁ biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined denoted diad axis dielectric dijk direction cosines displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ H₂ heat flow Hence hexagonal indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optic axis optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic photoelastic effect piezoelectric effect plane plate polarization positive principal axes produced pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal x₁ zero әт