Maxwell's equations in vacuum are written in a unit-independent form and then specialized to SI, Gaussian, CGS, and natural systems in both differential and integral versions.
On the analytical formulation of classical electromagnetic fields
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abstract
Three objections to the canonical analytical treatment of covariant electromagnetic theory are presented: (i) only half of Maxwell's equations are present upon variation of the fundamental Lagrangian; (ii) the trace of the canonical energy-momentum tensor is not equivalent to the trace of the observed energy-momentum tensor; (iii) the Belinfante symmetrization procedure exists separate from the analytical approach in order to obtain the known observed result. It is shown that the analytical construction from Noether's theorem is based on manipulations that were developed to obtain the compact forms of the theory presented by Minkowski and Einstein; presentations which were developed before the existence of Noether's theorem. By reformulating the fundamental Lagrangian, all of the objections are simultaneously relieved. Variation of the proposed Lagrangian yields the complete set of Maxwell's equations in the Euler-Lagrange equation of motion, and the observed energy-momentum tensor directly follows from Noether's theorem. Previously unavailable symmetries and identities that follow naturally from this procedure are also discussed.
fields
physics.class-ph 1years
2019 1verdicts
UNVERDICTED 1representative citing papers
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Electromagnetic Classical Field Theory in a Form Independent of Specific Units
Maxwell's equations in vacuum are written in a unit-independent form and then specialized to SI, Gaussian, CGS, and natural systems in both differential and integral versions.