Physical Properties of Crystals |
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Page 229
John Frederick Nye. the temperature gradient ; since temperature gradients not in the direc- tion of the current are relevant now , we have a transverse Thomson heat , in addition to the normal Thomson heat . The complete expression for ...
John Frederick Nye. the temperature gradient ; since temperature gradients not in the direc- tion of the current are relevant now , we have a transverse Thomson heat , in addition to the normal Thomson heat . The complete expression for ...
Page 230
... heat we take the crystal to have a symmetry that reduces [ Σik ] to the form ik and we orient it so that the ... Thomson heat . The rate of supply of heat needed to keep the tem- perature steady in an element of wire in which the ...
... heat we take the crystal to have a symmetry that reduces [ Σik ] to the form ik and we orient it so that the ... Thomson heat . The rate of supply of heat needed to keep the tem- perature steady in an element of wire in which the ...
Page 322
... heat , 228-30 . effect of crystal symmetry , 227 . in crystals , 224-30 . in isotropic conductors , 215-18 . in ... Thomson heat , 215-16 , 218 , 223 , 228-9 . Thomson heat tensor , 229 . Thomson relations , 216-18 . transverse Thomson ...
... heat , 228-30 . effect of crystal symmetry , 227 . in crystals , 224-30 . in isotropic conductors , 215-18 . in ... Thomson heat , 215-16 , 218 , 223 , 228-9 . Thomson heat tensor , 229 . Thomson relations , 216-18 . transverse Thomson ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 11 |
EQUILIBRIUM PROPERTIES | 51 |
16 | 59 |
23 other sections not shown
Common terms and phrases
angle anisotropic applied biaxial birefringence centre of symmetry Chapter coefficients 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 P₂ parallel Peltier permittivity perpendicular 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 symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial unit volume values wave normal wave surface x₁ Young's Modulus zero