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It's a lovely and very clear explanation!
Perhaps my only remaining question would be: How would you frame the
explanation in the lab frame instead?
In that frame we're maintaining
a charge separation across a finite gap d by essentially the Hall
effect.
Can I think of that like a capacitor? If so, how do I get
away with using the vacuum permittivity?
Can I think of that like a capacitor?
If so, how do I get
away with using the vacuum permittivity?