Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 4
... isotropic conductor and ( b ) an 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 ...
... isotropic conductor and ( b ) an 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 ...
Page 142
... isotropic materials . Using the ( §1 ) matrix given in Table 9 for an isotropic material , we may express the 8ij in terms of more familiar quantities , such as Young's Modulus and the Rigidity Modulus . First we write out the equations ...
... isotropic materials . Using the ( §1 ) matrix given in Table 9 for an isotropic material , we may express the 8ij in terms of more familiar quantities , such as Young's Modulus and the Rigidity Modulus . First we write out the equations ...
Page 215
... isotropic conductors . 1. Thermoelectric effects in isotropic conductors There are three thermoelectric effects in isotropic conductors : ( i ) The thermoelectric e.m.f. ( Seebeck effect ) . If a circuit is made of two different metals ...
... isotropic conductors . 1. Thermoelectric effects in isotropic conductors There are three thermoelectric effects in isotropic conductors : ( i ) The thermoelectric e.m.f. ( Seebeck effect ) . If a circuit is made of two different metals ...
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