A and ϕ inside a Faraday cage?

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SUMMARY

The discussion confirms that the vector potential A and the scalar potential ϕ are not necessarily zero inside a Faraday cage, similar to the electric field E and magnetic field B. The potentials are subject to gauge transformations, meaning their values depend on the chosen gauge fixing. The electromagnetic field can be zero in certain regions, but the potentials themselves do not have a unique physical interpretation. Instead, the observable quantities are the electric field E and magnetic field B, which are gauge-invariant and defined by the equations of motion in Maxwell's electrodynamics.

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Are A and ϕ always zero inside a Faraday cage, like E and B are?

If not, can its design be modified to accomplish that? If not, is there an analogous mechanism that'd always have A=0 and ϕ=0 inside?
 
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No. Same answer as your other thread. The potentials are only physical up to gauge transformations. It therefore makes little sense to talk about the value of the potentials (unless you fully specify the gauge fixing).
 
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If the em. field is zero somewhere, i.e., ##\vec{E}=\vec{B}=0##, then ##\Phi=\partial_t \chi/c## and ##vec{A}=-\vec{\nabla} \chi## for an arbitrary scalar field ##\chi##. The gauge potentials are not uniquely defined by the equations of motion describing a physical situation. That's, because Maxwell's electrodynamics is a gauge theory. The potentials do not have a specific physical meaning but the observable electromagnetic field ##\vec{E}=-\partial_t \vec{A}/c - \vec{\nabla} \chi##, ##\vec{B}=\vec{\nabla} \times \vec{A}##, which is a gauge-invariant quantity, has.
 

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