Non-relativistic limits of Maxwell's equations
arXiv:1303.5608 · doi:10.1088/0143-0807/34/4/859
Abstract
In 1973, Le Bellac and Levy-Leblond (Nuovo Cimento B 14, 217-234) discovered that Maxwell's equations possess two non-relativistic Galilei-covariant limits, corresponding to E >> cB (electric limit) or E << cB (magnetic limit). Here, we provide a systematic, yet simple, derivation of these two limits based on a dimensionless form of Maxwell's equations and an expansion of the electric and magnetic fields in a power series of some small parameters. Using this procedure, all previously known results are recovered in a natural and unambiguous way. Some further extensions are also proposed.
References in corpus (5)
- Numerical approximation of the Euler-Maxwell model in the quasineutral limit
- On some applications of Galilean electrodynamics of moving bodies
- The Galilean limits of Maxwell's equations
- The covariant formulation of Maxwell's equations expressed in a form independent of specific units
- From self-consistent covariant effective field theories to their Galilean-invariant counterparts
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