Electrodynamics of Continuous MediaCovers the theory of electromagnetic fields in matter, and the theory of the macroscopic electric and magnetic properties of matter. There is a considerable amount of new material particularly on the theory of the magnetic properties of matter and the theory of optical phenomena with new chapters on spatial dispersion and non-linear optics. The chapters on ferromagnetism and antiferromagnetism and on magnetohydrodynamics have been substantially enlarged and eight other chapters have additional sections. |
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Page 14
... dipole moment of the sphere is most easily found by comparing , with the potential Pr / r3 of an electric dipole field , whence P = R3E . PROBLEM 2. The same as Problem 1 , but for an infinite cylinder in a uniform transverse field ...
... dipole moment of the sphere is most easily found by comparing , with the potential Pr / r3 of an electric dipole field , whence P = R3E . PROBLEM 2. The same as Problem 1 , but for an infinite cylinder in a uniform transverse field ...
Page 34
... dipole moment of all the charges within the dielectric ; unlike the total charge , the total dipole moment need not be zero . By definition , it is the integral frpd V. Substituting p from ( 6.3 ) and again integrating over a volume ...
... dipole moment of all the charges within the dielectric ; unlike the total charge , the total dipole moment need not be zero . By definition , it is the integral frpd V. Substituting p from ( 6.3 ) and again integrating over a volume ...
Page 309
... dipole moment of the source . Since iw P , we have finally - E2 ( 1 ) · P1 = E1 ( 2 ) ⋅ P2 · ( 89.3 ) This form of the reciprocity theorem applies , of course , only to dipole emission . If the dipole moment of the source is zero , or ...
... dipole moment of the source . Since iw P , we have finally - E2 ( 1 ) · P1 = E1 ( 2 ) ⋅ P2 · ( 89.3 ) This form of the reciprocity theorem applies , of course , only to dipole emission . If the dipole moment of the source is zero , or ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
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angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ E₂ electric field electromagnetic electrons ellipsoid expression external field factor ferroelectric ferromagnet field H fluctuations fluid flux formula free energy frequency function given gives grad H₁ H₂ Hence incident induction integral isotropic Laplace's equation linear magnetic field magnetic moment Maxwell's equations medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities refraction relation respect result rotation satisfied scattering sin² SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ