Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 32
... hence determine graphically the magnitude and direction of the resultant current density . [ 8 ] Assuming the same electric field as in [ 6 ] , repeat the calculation [ 6 ] and the construction [ 7 ] using the x axes instead of the x ...
... hence determine graphically the magnitude and direction of the resultant current density . [ 8 ] Assuming the same electric field as in [ 6 ] , repeat the calculation [ 6 ] and the construction [ 7 ] using the x axes instead of the x ...
Page 70
... hence E ,, will be different . Since it is E , within the crystal that determines P by equation ( 5 ) , the two ... Hence P = Ko XEa a ( b ) A flat isotropic disk in d uniform field E , perpendicular to its faces . Inside the disk , κo ...
... hence E ,, will be different . Since it is E , within the crystal that determines P by equation ( 5 ) , the two ... Hence P = Ko XEa a ( b ) A flat isotropic disk in d uniform field E , perpendicular to its faces . Inside the disk , κo ...
Page 120
... Hence y X2 y d113 = X , X1 a b FIG . 7.2 . The point - group symmetry elements of class 42m showing ( a ) the conventional setting of the axes Ox1 , Ox1 , Ox , and ( b ) the setting obtained by a rotation of 45 ° about Ox ̧ . -d223 . In ...
... Hence y X2 y d113 = X , X1 a b FIG . 7.2 . The point - group symmetry elements of class 42m showing ( a ) the conventional setting of the axes Ox1 , Ox1 , Ox , and ( b ) the setting obtained by a rotation of 45 ° about Ox ̧ . -d223 . In ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
3 | 29 |
EQUILIBRIUM PROPERTIES | 51 |
23 other sections not shown
Common terms and phrases
angle anisotropic applied axial B₁ biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined denoted diad axis dielectric dijk direction cosines displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ H₂ 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 produced pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal x₁ zero әт