Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 76
... equations ( 18 ) and ( 19 ) we obtain , respectively , Poisson's equation and Laplace's equation : 226 226 026 + + = and P 226 მტ მიმი + ax32 - 0 . The known solutions of these two equations may therefore be imme- diately ...
... equations ( 18 ) and ( 19 ) we obtain , respectively , Poisson's equation and Laplace's equation : 226 226 026 + + = and P 226 მტ მიმი + ax32 - 0 . The known solutions of these two equations may therefore be imme- diately ...
Page 174
... equation ( 9 ) is short for nine equations ; in all , equations ( 9 ) and ( 10 ) stand for ten equations each with ten terms on the right - hand side . The four derivatives in ( 9 ) and ( 10 ) have physical meanings . Putting dT = 0 in ...
... equation ( 9 ) is short for nine equations ; in all , equations ( 9 ) and ( 10 ) stand for ten equations each with ten terms on the right - hand side . The four derivatives in ( 9 ) and ( 10 ) have physical meanings . Putting dT = 0 in ...
Page 201
... equation əhi div h = q or = Jxi ġ . Substituting for h , from equation ( 3 ) gives a2 T ku = -ġ , ( 11 ) a differential equation for the temperature T which is identical in form with the equation satisfied by the electrostatic potential ...
... equation əhi div h = q or = Jxi ġ . Substituting for h , from equation ( 3 ) gives a2 T ku = -ġ , ( 11 ) a differential equation for the temperature T which is identical in form with the equation satisfied by the electrostatic potential ...
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