Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 45
... value between S1 and S2 and reach their extreme values when R is at P and Q , that is , when the axes Ox coincide with the principal axes . We see too that ( S11 + S22 ) has the same value for all positions of the axes ; it is an ...
... value between S1 and S2 and reach their extreme values when R is at P and Q , that is , when the axes Ox coincide with the principal axes . We see too that ( S11 + S22 ) has the same value for all positions of the axes ; it is an ...
Page 187
... ( Values in rationalized m.k.s. units ) These values are necessarily very approximate . They do not take account of the spread in the values of the different components of each tensor ; nor do they indicate the considerable spread in the ...
... ( Values in rationalized m.k.s. units ) These values are necessarily very approximate . They do not take account of the spread in the values of the different components of each tensor ; nor do they indicate the considerable spread in the ...
Page 254
... values of ( 11-12 ) and ( 711-713 ) can be found . Such measurements of bire- fringence are comparatively easy to make . It may be shown , however , that measurements of birefringence alone cannot separate # 11 from # 12 , from π13 . It ...
... values of ( 11-12 ) and ( 711-713 ) can be found . Such measurements of bire- fringence are comparatively easy to make . It may be shown , however , that measurements of birefringence alone cannot separate # 11 from # 12 , from π13 . It ...
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