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Are Maxwell's equations approximations of something more general? How does one recover Maxwell's equations by taking the appropriate limit of the more general set of equations? Has it been worked out in the literature? Where can I find it?

In this article (which is on a completely different topic), Weinberg says that "They are understood today to be an approximation that is valid in a limited context (that of weak slowly-varying electric and magnetic fields)". What might he have in mind?

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Maxwell's equations are not approximations, they are the exact equations of motion of classical electromagnetism.

What Weinberg is likely referring to is that the classical equations of motion are of course only valid in situations where the classical limit of quantum electrodynamics is appropriate. For instance, at (very) high energies (above the Schwinger limit), you get significant contributions from quantum two-photon physics, contradicting e.g. the classical statement that two light beams shot "through" each other don't interact with each other.

Note that Maxwell's equations of motion are still the correct, non-approximative equations of motion for the quantum field, the "approximation" that fails is simply the approximation of a quantum theory by its corresponding classical theory, not something specific to electromagnetism as such.

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