Physical Properties of Crystals |
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Page 33
... angles are necessary to specify the direction of Ox1 , the latitude and longitude for example ; the new axes may still rotate about Ox1 , and so one further angle , an angle of rotation about Ox1 , is needed to fix them completely ...
... angles are necessary to specify the direction of Ox1 , the latitude and longitude for example ; the new axes may still rotate about Ox1 , and so one further angle , an angle of rotation about Ox1 , is needed to fix them completely ...
Page 97
... angle between them after deformation is π - 212 ( centre diagram of Fig . 6.6 ) . Note particularly that the tensor shear strain € 12 is one - half of the change in angle between the two elements . 2.1 . Homogeneous two - dimensional ...
... angle between them after deformation is π - 212 ( centre diagram of Fig . 6.6 ) . Note particularly that the tensor shear strain € 12 is one - half of the change in angle between the two elements . 2.1 . Homogeneous two - dimensional ...
Page 264
... angle between the wave normal and the optic axis , in agreement with the symmetry . Its variation is shown diagrammatically in Fig . 14.3 . Along the optic axis k = 1 , but it very rapidly falls off to small values and becomes zero at ...
... angle between the wave normal and the optic axis , in agreement with the symmetry . Its variation is shown diagrammatically in Fig . 14.3 . Along the optic axis k = 1 , but it very rapidly falls off to small values and becomes zero at ...
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