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 114
... magnetic field , unlike an electric field , does no work on charges moving in it ( since the force acting on a charge is perpendicular to its velocity ) . Hence , to calculate the change in the energy of the medium when a magnetic field ...
... magnetic field , unlike an electric field , does no work on charges moving in it ( since the force acting on a charge is perpendicular to its velocity ) . Hence , to calculate the change in the energy of the medium when a magnetic field ...
Page 182
... field is present . This means that no dissipation of energy occurs , whose ... magnetic properties . $ 54 . The superconductivity current Let us consider ... magnetic field . This can be seen as follows . The surface currents would ...
... field is present . This means that no dissipation of energy occurs , whose ... magnetic properties . $ 54 . The superconductivity current Let us consider ... magnetic field . This can be seen as follows . The surface currents would ...
Page 185
... magnetic field occur gradually over a fairly wide range of fields , so that there is no critical field in the sense here defined . Thus , at any temperature below the transition point , $ 55 185 The critical field §55 The critical field.
... magnetic field occur gradually over a fairly wide range of fields , so that there is no critical field in the sense here defined . Thus , at any temperature below the transition point , $ 55 185 The critical field §55 The critical field.
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