Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 83
... positive ends of the axes ( those shown in Fig . 5.1 ) . We denote by σ , the component of force in the + Ox , direction transmitted across that face of the cube which is perpendicular to Ox ,. † Note the sign convention : 012 , for ...
... positive ends of the axes ( those shown in Fig . 5.1 ) . We denote by σ , the component of force in the + Ox , direction transmitted across that face of the cube which is perpendicular to Ox ,. † Note the sign convention : 012 , for ...
Page 114
... positive ; it is true that he defines compressive stress components as positive ( p . 232 ) , but this seems to be an oversight , for throughout the rest of his book he treats them as positive when tensile . = - The array of di ...
... positive ; it is true that he defines compressive stress components as positive ( p . 232 ) , but this seems to be an oversight , for throughout the rest of his book he treats them as positive when tensile . = - The array of di ...
Page 125
... positive charge on compression ) . In left - handed quartz the positive end of the x axis develops a positive charge on extension . This convention evidently makes d11 negative for right - handed quartz and positive for left - handed ...
... positive charge on compression ) . In left - handed quartz the positive end of the x axis develops a positive charge on extension . This convention evidently makes d11 negative for right - handed quartz and positive for left - handed ...
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