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The potential difference between two points can be calculated along any path between them. I take a parallel plate capacitor and consider a small positive charge on the surface of the negatively charged sheet. I move it outside the sheet without doing any work as the net field inside a conductor is zero. Now, behind the sheet, the fields due to the two plates cancel each other perfectly. I move the charge away parallel to the plate, infinitely far away, when any fringes would've decayed away to nothing and move it to the other side. I repeat, bringing back the charge to the other plate. The two plates are seemingly at the same potential when they clearly are not. At what point of my process did I do work? What exactly is the potential at all points in space due to this system?

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  • $\begingroup$ There are field lines "behind" the plates of a real capacitor too, they don't cancel out due to the other plate. $\endgroup$
    – Triatticus
    Commented Jun 26, 2020 at 2:55

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Two infinite plates have perfectly parallel uniform field lines. For them, the field exactly cancels outside. But you can't go around infinite plates.

Finite plates at a large distance are like a dipole.

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