PAllen
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You don't need to solve for the Einstein tensor, since it is equal, up to constants, to the SET. You are effectively guessing an Einstein tensor when you guess an SET. Solving the pdiff system would give you a metric (or parameterized family of them) if your guess was good.Sciencemaster said:Alright, so if we construct a system in a way that's static, we could try solving the EFE's as a pdiff system of equations to find a time-independent metric (and Einstein Tensor)? Would this still work if the SET is piecewise, and does the SET itself have to be continuous I know the metric does, but does the SET have to be as well)?
I don't think it would be safe to make any guesses about the SET across the boundary. If you could pull off the pdiff solution for the SET of the material body part, then look for a general electrovac metric ansatz, assume this for the outside, and apply the junction conditions to constrain it. If your electrovac ansatz was not general enough, this may not be solvable.
I really doubt anyone has ever pulled this off analytically except for the case of spherical conductors or spherical charged fluid balls, bounded by an electrovac solution with spherical symmetry satisfying the junction conditions, and also satisfying EM consistency conditions across the boundary.
If you can find a full treatment of a solution for a charged ball, this would be at least your starting point for treating a different shape - which is much much more complicated.
If you are really serious, one reasonable place to start is Chapter 10, on Electromagnism in GR, in Synge's 1960 GR book. Specifically, the section on electrovac universes is exactly what you are trying to do (including an interior region of matter plus EM fields, and an exterior region of vacuum plus EM fields). This is a hard to find reference. Perhaps another science advisor knows of a more accessible reference for this material.
(Note: I think Synge uses junction conditions that predate Israel's, as Israel's work came after Synge's book).
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