Physical Properties of Crystals |
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Page 96
... rotation of PQ1 ; for the angle through which it turns is given by tan 0 = Suz Ax1 + Au1 Since we are only considering small displacements , u , and u , are small Q2 P ' Q2 Qi P Q1 FIG . 6.5 . Displacements in a small rigid- body rotation ...
... rotation of PQ1 ; for the angle through which it turns is given by tan 0 = Suz Ax1 + Au1 Since we are only considering small displacements , u , and u , are small Q2 P ' Q2 Qi P Q1 FIG . 6.5 . Displacements in a small rigid- body rotation ...
Page 98
... rotation about Ox , towards Ox , of a line element parallel to Ox2 , e21 is the rotation about Ox , towards Ox , of a line element parallel to Ox1 , and similarly for the other Cij If the body merely undergoes a rotation with no strain ...
... rotation about Ox , towards Ox , of a line element parallel to Ox2 , e21 is the rotation about Ox , towards Ox , of a line element parallel to Ox1 , and similarly for the other Cij If the body merely undergoes a rotation with no strain ...
Page 261
... rotation of the plane of polarization is clockwise as seen by an observer whose eye the light is entering ; as is customary , we call this a right - handed rotation and define it as positive ( provided right- handed axes are chosen ) ...
... rotation of the plane of polarization is clockwise as seen by an observer whose eye the light is entering ; as is customary , we call this a right - handed rotation and define it as positive ( provided right- handed axes are chosen ) ...
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