Physical Properties of Crystals |
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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 248
... number and j as the row number , which is the reverse of the usual procedure ... independent photoelastic coefficients . Since , in equation ( 14 ) , AB1 ... number of independent coeffi- cients from 34 = 81 to 36 , and they make possible ...
... number and j as the row number , which is the reverse of the usual procedure ... independent photoelastic coefficients . Since , in equation ( 14 ) , AB1 ... number of independent coeffi- cients from 34 = 81 to 36 , and they make possible ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 11 |
EQUILIBRIUM PROPERTIES | 51 |
16 | 59 |
23 other sections not shown
Common terms and phrases
angle anisotropic applied biaxial birefringence centre of symmetry Chapter coefficients conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined deformation denoted diad axis dielectric dijk displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ 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 P₂ parallel Peltier permittivity perpendicular photoelastic effect piezoelectric effect plane plate polarization positive principal axes 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 unit volume values wave normal wave surface x₁ Young's Modulus zero