Physical Properties of Crystals |
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Page 25
... magnitude of a property in a given direction is one that needs careful definition , because of the lack of parallelism between the vectors involved . Take electrical conductivity as an example ( Fig . 1.7 ) . We apply a field E in a ...
... magnitude of a property in a given direction is one that needs careful definition , because of the lack of parallelism between the vectors involved . Take electrical conductivity as an example ( Fig . 1.7 ) . We apply a field E in a ...
Page 86
... magnitude pdx5 . Hence , as the element becomes infinitesimally small , unless - 032-023 + G1 0 , ( 3 ) Ö1 must ... magnitude smaller than the lever arm for the shear forces and so the terms may be neglected . ( These forces actually ...
... magnitude pdx5 . Hence , as the element becomes infinitesimally small , unless - 032-023 + G1 0 , ( 3 ) Ö1 must ... magnitude smaller than the lever arm for the shear forces and so the terms may be neglected . ( These forces actually ...
Page 187
... magnitude of the effects . The magnitude of all the possible interactions between the crystal properties we are considering is given when the magnitudes of the partial differential coefficients in equations ( 27 ) , ( 28 ) , ( 29 ) are ...
... magnitude of the effects . The magnitude of all the possible interactions between the crystal properties we are considering is given when the magnitudes of the partial differential coefficients in equations ( 27 ) , ( 28 ) , ( 29 ) are ...
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