Physical Properties of Crystals |
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Page 99
... represented by an axial vector ( Ch . II , § 2 ) , and an axial vector is equivalent to an antisymmetrical second ... represented by the first two terms on the right - hand side of ( 10 ) , from the part that is due to strain ...
... represented by an axial vector ( Ch . II , § 2 ) , and an axial vector is equivalent to an antisymmetrical second ... represented by the first two terms on the right - hand side of ( 10 ) , from the part that is due to strain ...
Page 169
... represented by the ( 3 × 1 ) matrix I. Then , in this direction , the magnitude S of a symmetrical second - rank tensor property given by the ( 3 × 3 ) matrix S is S = I , SI . ( § 6 ) A transformation of axes may be represented by the ...
... represented by the ( 3 × 1 ) matrix I. Then , in this direction , the magnitude S of a symmetrical second - rank tensor property given by the ( 3 × 3 ) matrix S is S = I , SI . ( § 6 ) A transformation of axes may be represented by the ...
Page 242
... represented by the double - headed arrow through the origin . The refractive index is proportional to the square root of the slope of curve B at the origin . Now suppose that a static electric field E is applied in the direction we are ...
... represented by the double - headed arrow through the origin . The refractive index is proportional to the square root of the slope of curve B at the origin . Now suppose that a static electric field E is applied in the direction we are ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 11 |
EQUILIBRIUM PROPERTIES | 45 |
PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY | 53 |
20 other sections not shown
Common terms and phrases
angle anisotropic applied biaxial birefringence centre of symmetry Chapter coefficients components 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 parallel Peltier permittivity perpendicular photoelastic 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 suffixes symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal wave surface x₁ Young's Modulus zero ат