Electrodynamics of Continuous Media: Volume 8Covers the theory of electromagnetic fields in matter, and the theory of 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. |
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Page 40
... external field imposed , and the second , which vanishes at infinity , gives the required change in potential due to the sphere ( cf. §3 , Problem 1 , solution ) . Inside the sphere , we seek the field potential in the form = Br , the ...
... external field imposed , and the second , which vanishes at infinity , gives the required change in potential due to the sphere ( cf. §3 , Problem 1 , solution ) . Inside the sphere , we seek the field potential in the form = Br , the ...
Page 184
... external magnetic field , the total magnetic flux is composed of the flux LJ / c and the flux of the external field . A very important property of a superconducting ring is that , even if the external field and the current vary , the ...
... external magnetic field , the total magnetic flux is composed of the flux LJ / c and the flux of the external field . A very important property of a superconducting ring is that , even if the external field and the current vary , the ...
Page 185
... external field is completely determined by the n - 1 total currents J. The relation ( 54.5 ) becomes the system of equations Σ Lab Jb + ( e ) = 0 , Φ Φαο · a b ( 54.6 ) These equations hold , not only for any external field , but also ...
... external field is completely determined by the n - 1 total currents J. The relation ( 54.5 ) becomes the system of equations Σ Lab Jb + ( e ) = 0 , Φ Φαο · a b ( 54.6 ) These equations hold , not only for any external field , but also ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
Copyright | |
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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 equation expression external field 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 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