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0 electrodynamics Beltrami vector fields

In this final section, it is shown that the three magnetic field components of electromagnetic radiation in 0(3) electrodynamics are Beltrami vector fields, illustrating the fact that conventional Maxwell-Heaviside electrodynamics are incomplete. Therefore Beltrami electrodynamics can be regarded as foundational, structuring the vacuum fields of nature, and extending the point of view of Heaviside, who reduced the original Maxwell equations to their presently accepted textbook form. In this section, transverse plane waves are shown to be solenoidal, complex lamellar, and Beltrami, and to obey the Beltrami equation, of which B is an identically nonzero solution. In the Beltrami electrodynamics, therefore, the existence of the transverse 1 = implies that of , as in 0(3) electrodynamics. [Pg.250]

BELTRAMI VECTOR FIELDS IN ELECTRODYNAMICS—A REASON FOR REEXAMINING THE STRUCTURAL FOUNDATIONS OF CLASSICAL FIELD PHYSICS ... [Pg.525]

When we consider time-harmonic electrodynamics in more general media (chiral-biisotropic), A. Lakhtakia also underscored the importance of the Beltrami field condition [54], In particular, he found that time-harmonic EM fields in a homogeneous reciprocal biisotropic medium are circularly polarized, and must be described by Beltrami vector fields. [Pg.549]


See other pages where 0 electrodynamics Beltrami vector fields is mentioned: [Pg.527]    [Pg.529]    [Pg.531]    [Pg.533]    [Pg.534]    [Pg.535]    [Pg.537]    [Pg.539]    [Pg.541]    [Pg.543]    [Pg.545]    [Pg.547]    [Pg.549]    [Pg.551]    [Pg.553]    [Pg.555]    [Pg.556]    [Pg.557]    [Pg.559]    [Pg.561]    [Pg.563]    [Pg.565]    [Pg.567]    [Pg.569]   
See also in sourсe #XX -- [ Pg.253 , Pg.254 , Pg.255 , Pg.256 ]




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