PeterDonis
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PeterDonis said:Now, the quick summary of what I think GR actually says about this scenario
On re-reading, it may be confusing to state things in terms of coordinates and frames as I did. So in case it's needed to improve clarity, let me re-state everything in terms of how it would actually be measured in the scenario we are considering.
The charge on the capacitor inside the shell is q. Since this charge is only "visible" between the plates, if we are going to measure it using Gauss's Law (which is the point at issue), we have to, as I said previously, use a closed surface that encloses just one plate, measure the electric field normal to each small segment of that surface, and integrate over the entire surface. The electric field is nonzero only between the plates, and (in the idealized case) is exactly uniform and exactly normal to the plates, so the measured charge will be q = E * A, where E is the electric field and A is the plate area (in "proper" units). Note that, as before, I am leaving out constant factors of epsilon_0 or 4 pi or whatever that depend only on the units we're using.
One could, I suppose, try to concoct a way of "remotely" measuring the charge, by "remotely" measuring either the electric field or the area. But how would you do that directly? You could measure the electric field indirectly, by measuring energy (we'll discuss that below), but that requires you to "interpret" what the energy measurement says about the electric field. The whole point here is to get down to the direct observables, eliminating all indirect "interpretation" steps. So one way of putting the fact that the charge is q "regardless of which coordinates you use" would be to say that there is only one way to *measure* q, which is locally; there is no way for an observer at infinity to directly measure q on the capacitor inside the shell.
The energy stored in the capacitor, as measured anywhere inside the shell, is W = E * d * q = E^2 * d * A, where d is the plate separation (again in "proper" units). As our direct measurement of energy, we will adopt Q-reeus' method of putting a known charge on the plates (measured using Gauss's Law as above), and then measuring the work required to separate the plates by a proper distance d, by means of a linkage between the "source" of the work and the capacitor itself. If we do this using a "source" of work anywhere inside the shell, we will get W as above.
The energy stored in the capacitor, as measured at infinity, is W sqrt(J). This is easy to see just by comparing the measurement at infinity with the measurement inside the shell, given above. The measurement at infinity requires a linkage extending from infinity to the capacitor inside the shell, and any work done through that linkage will be "redshifted" by a factor of sqrt(J). More precisely, it will be redshifted by a factor sqrt(ratio of g_tt inside shell to g_tt at infinity), but since g_tt at infinity is 1, the ratio is just sqrt(g_tt inside shell) = sqrt(J). (Btw, this analysis also shows us that the reason why the energy measurement gives W anywhere inside the shell, is that g_tt is *constant* inside the shell--if it varied there, the energy measurement would vary too, depending on where the "source" of the work was relative to the capacitor. Only in the limiting case of a truly local inertial frame, where g_tt can be considered constant throughout the "patch" of spacetime under consideration, will we always get W as the energy measurement.)
The voltage on the capacitor, measured anywhere inside the shell, is, as is obvious from the above, V = E * d. The obvious direct measurement of voltage would simply be to put a voltmeter across the capacitor plates, which amounts to measuring the work required to move a test charge from one plate to the other against the electric field. Note that this is *not* the same as the total energy stored in the capacitor; it is better viewed as a "cross check" of sorts. In other words, once all three measurements are taken (charge, energy, and voltage), we must have W = V * q, even though all three were measured using independent methods.
As with charge above, however, I do not see any way to *directly* measure the voltage on the capacitor "at infinity"; the only way I see to do it is indirectly, by measuring energy at infinity and then deducing, since W = V * q and q is the same, that V must "redshift" the same way W does. However, this does open up a question: since both V and q can't be measured directly "at infinity", could we adopt an interpretation of the energy "redshifting" that has q "redshifting" *instead* of V? In other words, we would say that V(at infinity) = V and q(at infinity) = q sqrt(J), so W(at infinity) = V(at infinity) * q(at infinity) = W sqrt(J) still holds.
I personally don't see any reason to adopt this interpretation, but I can't say on a quick look that it's actually inconsistent--although I haven't checked it with the math, it's quite possible that there would be an inconsistency (or more precisely, that there would be no way to consistently formulate the "q redshifting instead of V" interpretation mathematically). However, one thing I do want to note is that this is *not* what Q-reeus is proposing! Q-reeus is saying that q(at infinity) = q sqrt(J) *and* V(at infinity) = V sqrt(J) (because he says the E field "redshifts" *and* charge "redshifts"). I don't see how to fit this in with the fact that W = V * q should hold.