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 4
... e = Co , where C is the capacitance , which in order of magnitude is equal to the linear dimension of the body . The converse relations , giving the potentials in terms of the charges , are Q2 = Σ C - 1ab2 b Φαξ ( 2.4 ) where the ...
... e = Co , where C is the capacitance , which in order of magnitude is equal to the linear dimension of the body . The converse relations , giving the potentials in terms of the charges , are Q2 = Σ C - 1ab2 b Φαξ ( 2.4 ) where the ...
Page 32
... E , its energy is given by formula ( 2.14 ) . The extending pressure is therefore AP = Ex i ( 5.13 ) PROBLEMS ... co ( 1 − a / r ) . The required force of interaction F is the Coulomb repulsion between the charge e on the conductor and ...
... E , its energy is given by formula ( 2.14 ) . The extending pressure is therefore AP = Ex i ( 5.13 ) PROBLEMS ... co ( 1 − a / r ) . The required force of interaction F is the Coulomb repulsion between the charge e on the conductor and ...
Page 97
... Co / e , and we shall write this henceforward as simply . In a homogeneous metal , the change amounts to the adding of an unimportant constant to the potential . Accordingly , the " field " E = - grad ( which we shall use henceforward ) ...
... Co / e , and we shall write this henceforward as simply . In a homogeneous metal , the change amounts to the adding of an unimportant constant to the potential . Accordingly , the " field " E = - grad ( which we shall use henceforward ) ...
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