Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 3
... quantities , such as the density or the temperature of a body , which are not connected in any way with direction . With the usual definitions of density and temperature it is meaningless to speak of measuring these quantities in any ...
... quantities , such as the density or the temperature of a body , which are not connected in any way with direction . With the usual definitions of density and temperature it is meaningless to speak of measuring these quantities in any ...
Page 21
... quantities , taking our measurements in the same directions as before , relative to the fixed axes . If the relation between the measured quantities is unchanged , we say that the property in question , in this particular crystal ...
... quantities , taking our measurements in the same directions as before , relative to the fixed axes . If the relation between the measured quantities is unchanged , we say that the property in question , in this particular crystal ...
Page 40
... quantities symbolized by Fig . 2.2 a and those symbolized by Fig . 2.26 , simply reflect each symbol in a plane perpendicular to its length . This evidently reverses quantities which are polar vectors , but leaves unchanged quantities ...
... quantities symbolized by Fig . 2.2 a and those symbolized by Fig . 2.26 , simply reflect each symbol in a plane perpendicular to its length . This evidently reverses quantities which are polar vectors , but leaves unchanged quantities ...
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