Physical Properties of Crystals |
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Page 111
... applied in turn along Оx , and Ox , physical meanings may be attached to the other dijk coefficients in which j = k . Suppose now that a pure shear stress 012 is applied . We have to remember that , if body - torques are ignored ( p ...
... applied in turn along Оx , and Ox , physical meanings may be attached to the other dijk coefficients in which j = k . Suppose now that a pure shear stress 012 is applied . We have to remember that , if body - torques are ignored ( p ...
Page 132
... applied parallel to one set of edges , it will not only stretch in the direction of the tension but it may also ... applied , remembering that without body - torquest 12 cannot be applied without σ21 , we should have € 11 = = S1112 12 + ...
... applied parallel to one set of edges , it will not only stretch in the direction of the tension but it may also ... applied , remembering that without body - torquest 12 cannot be applied without σ21 , we should have € 11 = = S1112 12 + ...
Page 246
... applied parallel to a 3- , 4- or 6 - fold axis will give an optically uniaxial crystal with the optic axis parallel to the stress . On the other hand , a uniaxial stress applied a Ꮧ , b FIG . 13.10 . A cubic crystal of class 23. ( a ) ...
... applied parallel to a 3- , 4- or 6 - fold axis will give an optically uniaxial crystal with the optic axis parallel to the stress . On the other hand , a uniaxial stress applied a Ꮧ , b FIG . 13.10 . A cubic crystal of class 23. ( a ) ...
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