I Orbital Period In General Relativity

dsaun777
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What is the orbital period in General Relativity using the Schwarzschild metric? In classical mechanics, it is something like
T=2pi(GnM/a3). Where a is the semi-major axis, this is for a small body orbiting a larger one. I think I have an idea but I am not 100% sure. I am interested in an outside observer far away viewing a small particle m in orbit of some mass M.
 
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dsaun777 said:
What is the orbital period in General Relativity using the Schwarzschild metric?
For a circular orbit, it's the Kepler's Third Law expression with the Schwarzschild ##r## plugged in as the orbital radius. Note that this is the case even though ##r## is not the same as the physical distance from the center of mass of the central body.
 
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PeterDonis said:
For a circular orbit, it's the Kepler's Third Law expression with the Schwarzschild ##r## plugged in as the orbital radius. Note that this is the case even though ##r## is not the same as the physical distance from the center of mass of the central body.
Yeah, its the areal radius found by integrating over the radial coordinate from r to rs dr using the metric components related to radial coordinates.
 
dsaun777 said:
Yeah, its the areal radius
Yes, but...

dsaun777 said:
found by integrating over the radial coordinate from r to rs dr using the metric components related to radial coordinates.
...no, that's not what the areal radius is. The areal radius is ##r = \sqrt{A / 4 \pi}##, where ##A## is the surface area of the 2-sphere labeled by ##r## that is centered on the central mass.
 
From $$0 = \delta(g^{\alpha\mu}g_{\mu\nu}) = g^{\alpha\mu} \delta g_{\mu\nu} + g_{\mu\nu} \delta g^{\alpha\mu}$$ we have $$g^{\alpha\mu} \delta g_{\mu\nu} = -g_{\mu\nu} \delta g^{\alpha\mu} \,\, . $$ Multiply both sides by ##g_{\alpha\beta}## to get $$\delta g_{\beta\nu} = -g_{\alpha\beta} g_{\mu\nu} \delta g^{\alpha\mu} \qquad(*)$$ (This is Dirac's eq. (26.9) in "GTR".) On the other hand, the variation ##\delta g^{\alpha\mu} = \bar{g}^{\alpha\mu} - g^{\alpha\mu}## should be a tensor...
OK, so this has bugged me for a while about the equivalence principle and the black hole information paradox. If black holes "evaporate" via Hawking radiation, then they cannot exist forever. So, from my external perspective, watching the person fall in, they slow down, freeze, and redshift to "nothing," but never cross the event horizon. Does the equivalence principle say my perspective is valid? If it does, is it possible that that person really never crossed the event horizon? The...

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