Physical Properties of Crystals |
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Page 105
... represents the displacement of a point x ; in a deformed body , we define the tensor [ e ;; ] by lij = dui dx ; The symmetrical part of this tensor , with components = Eij Į ( eij + eji ) , represents the strain at the point ; the ...
... represents the displacement of a point x ; in a deformed body , we define the tensor [ e ;; ] by lij = dui dx ; The symmetrical part of this tensor , with components = Eij Į ( eij + eji ) , represents the strain at the point ; the ...
Page 242
... represents the relation between D and E for changes at optical frequencies . Suppose , then , that a light wave ... represented by the double - headed arrow through the origin . The refractive index is proportional to the square root of ...
... represents the relation between D and E for changes at optical frequencies . Suppose , then , that a light wave ... represented by the double - headed arrow through the origin . The refractive index is proportional to the square root of ...
Page 259
... represents the linear photoelastic effect , and the term bЕ represents the Kerr effect ; both these effects can exist in crystals of any symmetry . By writing down the appropriate derivatives , and using the thermodynamic relations of ...
... represents the linear photoelastic effect , and the term bЕ represents the Kerr effect ; both these effects can exist in crystals of any symmetry . By writing down the appropriate derivatives , and using the thermodynamic relations of ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 11 |
EQUILIBRIUM PROPERTIES | 45 |
PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY | 53 |
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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