What Happens to Matter Inside a Black Hole's Infinite Density?

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If an object is infinitely dense, does this simply mean that there is no empty space within the object? I'm hung up on the fact that you can't possibly get denser than infinite density; what is stopping a black hole from getting even denser? What happens to atoms once they're under such intense gravitational pressure? !
 
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It is not believed that "infinite density" exists in the real world. It is a mathematical fiction that is the result of some model's calculations and is therefore taken as a sign that the model breaks down at the point where it gives infinity as a result.

For example, the most standard model of a black hole says there is a singularity at the center that has zero volume and all of the mass of the black hole and therefore infinite density, but what that really means is that we don't understand the black hole singularity. A successful theory of quantum gravity will likely give a different answer for what the singularity of a black hole is.
 
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...
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...
ASSUMPTIONS 1. Two identical clocks A and B in the same inertial frame are stationary relative to each other a fixed distance L apart. Time passes at the same rate for both. 2. Both clocks are able to send/receive light signals and to write/read the send/receive times into signals. 3. The speed of light is anisotropic. METHOD 1. At time t[A1] and time t[B1], clock A sends a light signal to clock B. The clock B time is unknown to A. 2. Clock B receives the signal from A at time t[B2] and...

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