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Oct 5, 2012 at 6:48 history edited Qmechanic CC BY-SA 3.0
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Oct 5, 2012 at 6:37 history edited Qmechanic CC BY-SA 3.0
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Oct 5, 2012 at 0:12 vote accept Deep Blue
Oct 5, 2012 at 7:21
Oct 5, 2012 at 0:09 comment added Deep Blue I'll see if I can get that result this evening.
Oct 4, 2012 at 23:39 comment added Qmechanic Right, after you impose the appropriate initial condition, then your FT formula for $Q(t)$ must be equivalent to the manifestly causal formula in my answer.
Oct 4, 2012 at 23:20 comment added Deep Blue I agree, but does that solution not solve the original equation? Since the equation is causal, I expect the solution to maintain that property. I remember from school that when solving wave equations in classical EM, a delta function pops out during integration and enforces this causality (this raises an interesting question of what would happen when it is solved on a finite interval where the wavenumbers are discrete, but that's for another time) - but I can't see a way that such a causality-ex-machina would show up in any general problem.
Oct 4, 2012 at 23:08 comment added Qmechanic The very first step: to use an object (the FT) that depends on the far future, cf. section I.
Oct 4, 2012 at 23:01 comment added Deep Blue I agree that the problem may be solved like you have wrote, but what step goes wrong in the FT approach that seems to break causality? If the solution I outlined above it valid, what would happen if I try to evaluate it for some input function? I suspect that if I switch the order of integration, the first (homogeneous) solution term you wrote may pop out from the transform solution, but I've yet to check it out. Also, as I said in, I'm interested in this difficulty in a more general situation, and only used the RC circuit to illustrate the problem.
Oct 4, 2012 at 20:50 history edited Qmechanic CC BY-SA 3.0
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Oct 4, 2012 at 20:41 history edited Qmechanic CC BY-SA 3.0
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Oct 4, 2012 at 20:06 history answered Qmechanic CC BY-SA 3.0