Physical Properties of Crystals |
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Page 11
... relation between p and q in a crystal . The corresponding equation for an iso- tropic body would be = Pi Tqi ( 10 ) ... relation between them . If the coefficients are given for one particular choice of axes the property is completely ...
... relation between p and q in a crystal . The corresponding equation for an iso- tropic body would be = Pi Tqi ( 10 ) ... relation between them . If the coefficients are given for one particular choice of axes the property is completely ...
Page 21
... relation between certain measurable quantities associated with the crystal . For example , the elasticity of a crystal is a certain relation between a homogeneous stress and a homogeneous strain in the crystal . Now suppose we wish to ...
... relation between certain measurable quantities associated with the crystal . For example , the elasticity of a crystal is a certain relation between a homogeneous stress and a homogeneous strain in the crystal . Now suppose we wish to ...
Page 205
... relation k¡¡ = kji During the foregoing discussion of heat conduction in anisotropic crystals we assumed the validity of the relation k1j = kj 、· kji . ( 4 ) That this assumption is justifiable is by no means obvious . It asserts , for ...
... relation k¡¡ = kji During the foregoing discussion of heat conduction in anisotropic crystals we assumed the validity of the relation k1j = kj 、· kji . ( 4 ) That this assumption is justifiable is by no means obvious . It asserts , for ...
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