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Free-space Maxwell equations current density

As noted elsewhere [67], Eq. (14) means that the continuity condition does not prohibit the existence of an electromagnetic current density J in free space. It is stressed that Eq. (14) is a mathematical prediction of Maxwell s equations, completely independent of any interpretation. [Pg.346]

These four vector relations compactly summarize the experimental laws describing all known electrical and magnetic phenomena. In these expressions, p is the electric charge density, J, the current density, E, the electric field and B, the magnetic induction. Maxwell s equations in free space (in the absence of dielectric or magnetic media) can be written... [Pg.176]

The spatial dependence of the electric field E(x, y, z) and the magnetic field H(x, y, z) of an optical waveguide is determined by Maxwell s equations. We assume an implicit time dependence exp( — iwt) in the field vectors, current density J and charge density a. The dielectric constant s(x, y, z) is related to the refractive index n(x, y, z) by e = n CQ, where Eq is the dielectric constant of free space. For the nonmagnetic materials which normally constitute an optical waveguide, the magnetic permeability p is very nearly equal to the free-space value Pq. Thus for convenience we assume p = Po throughout this book unless otherwise stated. Under these conditions. Maxwell s equations are expressible in the form[l]... [Pg.590]


See other pages where Free-space Maxwell equations current density is mentioned: [Pg.163]    [Pg.339]    [Pg.11]   
See also in sourсe #XX -- [ Pg.349 ]




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