Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 113
... number of independent moduli . Matrix notation A general third - rank tensor , as we have seen , has 33 27 inde- pendent components . When the components are written out in full they form ... number of independent moduli Matrix notation.
... number of independent moduli . Matrix notation A general third - rank tensor , as we have seen , has 33 27 inde- pendent components . When the components are written out in full they form ... number of independent moduli Matrix notation.
Page 122
... independent , but only the total number of independent ones . The listing of the independent components in each class by group theoretical methods has been studied by Fumi ( 1952 d ) and by Fieschi and Fumi ( 1953 ) , who give further ...
... independent , but only the total number of independent ones . The listing of the independent components in each class by group theoretical methods has been studied by Fumi ( 1952 d ) and by Fieschi and Fumi ( 1953 ) , who give further ...
Page 293
... sixth - rank tensor is discussed by Mason ( 1951 ) [ see also errata in Mason ( 1952 ) ] . TABLE 25 Number of independent coefficients Class symbol Inter- Schoen- The number of independent coefficients in the 32 crystal classes.
... sixth - rank tensor is discussed by Mason ( 1951 ) [ see also errata in Mason ( 1952 ) ] . TABLE 25 Number of independent coefficients Class symbol Inter- Schoen- The number of independent coefficients in the 32 crystal classes.
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