I I don't see how a black hole's event horizon can be crossed

Foretranimal
Messages
1
Reaction score
3
TL;DR Summary
Is it possible that Eienstien's equivalence principle does not apply to the perspective of someone falling through the event horizon of a black hole, because that perspective does not and cannot exist?
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 thing I have always read is that when the in-faller crosses, they feel nothing special. But this paradox seems to assume the crossing happens. If the crossing never happens, is there an information paradox at all?

If it takes forever to cross the event horizon, and a black hole's existence is less than forever, would the black hole evaporate before that unfortunate person crosses the horizon?

It seems more like the event horizon has no "there" or "inside" the event horizon - the horizon is an asymptotic limit of what exists. There is no inside, like there is no "before" the Big Bang. If you remove the assumption, there was a crossing, is there still a paradox?

I have no expertise in this area, so there may well be something basic I am just missing.
 
Physics news on Phys.org
Foretranimal said:
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.
The standard Schwarzschild coordinates that you refer to in the second statement are on a different manifold than the Hawking spacetime for the first statement.
 
In this video I can see a person walking around lines of curvature on a sphere with an arrow strapped to his waist. His task is to keep the arrow pointed in the same direction How does he do this ? Does he use a reference point like the stars? (that only move very slowly) If that is how he keeps the arrow pointing in the same direction, is that equivalent to saying that he orients the arrow wrt the 3d space that the sphere is embedded in? So ,although one refers to intrinsic curvature...
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...
So, to calculate a proper time of a worldline in SR using an inertial frame is quite easy. But I struggled a bit using a "rotating frame metric" and now I'm not sure whether I'll do it right. Couls someone point me in the right direction? "What have you tried?" Well, trying to help truly absolute layppl with some variation of a "Circular Twin Paradox" not using an inertial frame of reference for whatevere reason. I thought it would be a bit of a challenge so I made a derivation or...
Back
Top