Physical Properties of Crystals: Their Representation by Tensors and Matrices |
From inside the book
Results 1-3 of 55
Page 108
... zero . The angle between these directions and the Ox , axis is easily found . If ( 1,2,3 ) are the direction cosines of one of the lines of zero expansion we have ( 13 + 13 ) α1 + 13α2 = ( 1-13 ) α1 + 13α = 0 . cos , we obtain Since l ...
... zero . The angle between these directions and the Ox , axis is easily found . If ( 1,2,3 ) are the direction cosines of one of the lines of zero expansion we have ( 13 + 13 ) α1 + 13α2 = ( 1-13 ) α1 + 13α = 0 . cos , we obtain Since l ...
Page 185
... zero ) during the change is thus the normal component of D and the transverse components of E. In this way we see that , while making the surface of the crystal an equipotential ensures that E is zero , isolating the crystal does not ...
... zero ) during the change is thus the normal component of D and the transverse components of E. In this way we see that , while making the surface of the crystal an equipotential ensures that E is zero , isolating the crystal does not ...
Page 211
... zero † and write kij = kji . We are not forced to do so but it is permissible . ( 4 ) One of the consequences of not accepting ( 4 ) would be that we should have to assume that the conductivity of a vacuum is not zero . To see this ...
... zero † and write kij = kji . We are not forced to do so but it is permissible . ( 4 ) One of the consequences of not accepting ( 4 ) would be that we should have to assume that the conductivity of a vacuum is not zero . To see this ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
EQUILIBRIUM PROPERTIES | 51 |
ELECTRIC POLARIZATION | 68 |
18 other sections not shown
Common terms and phrases
angle anisotropic applied axial vector centre of symmetry Chapter coefficients conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals defined denoted diad axis dielectric dijk direction cosines dummy suffix elastic electric field ellipsoid equation example force given grad H₁ H₂ heat flow Hence hexagonal homogeneous indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic effect piezoelectric effect plane plate polarization principal axes produced pyroelectric pyroelectric effect quantities radius vector referred refractive index relation representation quadric represented right-handed rotation S₁ scalar second-rank tensor set of axes shear strain stress suffix notation surface susceptibility symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values x₁ Young's Modulus zero