Physical Properties of Crystals: Their Representation by Tensors and Matrices |
From inside the book
Results 1-3 of 29
Page xiv
Their Representation by Tensors and Matrices John Frederick Nye. potentially anisotropic , and then we can go on to prove that , for certain properties , they are isotropic . All crystals are anisotropic for some of their properties . In ...
Their Representation by Tensors and Matrices John Frederick Nye. potentially anisotropic , and then we can go on to prove that , for certain properties , they are isotropic . All crystals are anisotropic for some of their properties . In ...
Page 4
... anisotropic conductor . is isotropic and obeys Ohm's Law , j is parallel to E ( Fig . 1.1a ) , and the magnitude of j is proportional to the magnitude of E. We write j = σE , ( 1 ) where σ is the conductivity . If , with axes Ox1 , Ox2 ...
... anisotropic conductor . is isotropic and obeys Ohm's Law , j is parallel to E ( Fig . 1.1a ) , and the magnitude of j is proportional to the magnitude of E. We write j = σE , ( 1 ) where σ is the conductivity . If , with axes Ox1 , Ox2 ...
Page 202
... anisotropic medium . Start with the solution to an appropriate heat - flow problem in an isotropic medium of conductivity ( k , ką ką ) 1 . We form a picture of the solution by imagining the sources , the boundaries , the isothermals ...
... anisotropic medium . Start with the solution to an appropriate heat - flow problem in an isotropic medium of conductivity ( k , ką ką ) 1 . We form a picture of the solution by imagining the sources , the boundaries , the isothermals ...
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