Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 153
... zero , the equation AB = 0 ( 0 standing for the null matrix all of whose elements are zero ) does not necessarily imply that either A or B is zero . Similarly , for the magnetic permeability , B = μH § 2 153 THE MATRIX METHOD Crystal ...
... zero , the equation AB = 0 ( 0 standing for the null matrix all of whose elements are zero ) does not necessarily imply that either A or B is zero . Similarly , for the magnetic permeability , B = μH § 2 153 THE MATRIX METHOD Crystal ...
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 |
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