- #1
Tomas Vencl
- 66
- 13
- TL;DR Summary
- Inside observer view of a collapsing shell
let's consider spherically symmetrical thin shell of dust, which is collapsing under its own gravity. There are no other forces as pressure or so except gravity, and particles of shell (dust) are in free fall. The shell has total mass M and collapse starts from rest state with diameter of the shell much larger than its Schwarzschild radius. During all collapse the symmetry remains.
Now consider observer (a) with negligible mass in the center of the shell. The observer has a clock and measures its propper time t(a). The observer also has a flashlight, and can send signals and receive reflected signals from inner wall of the shell.
Until the observer is absorbed (collapsed) by the shell, he is still in flat spacetime and he can make some measurements.
If he will measure (or calculate) the "velocity" of inner wall of collapsing shell (meaning dr/dt(a) ,what he will measure/calculate ? Mainly after the shell passes the Schwarzschild radius ? Does the defined "speed" exceeds c, or what are the limits ?
Or generally, what observer (a) can see during collapse ?
Now consider observer (a) with negligible mass in the center of the shell. The observer has a clock and measures its propper time t(a). The observer also has a flashlight, and can send signals and receive reflected signals from inner wall of the shell.
Until the observer is absorbed (collapsed) by the shell, he is still in flat spacetime and he can make some measurements.
If he will measure (or calculate) the "velocity" of inner wall of collapsing shell (meaning dr/dt(a) ,what he will measure/calculate ? Mainly after the shell passes the Schwarzschild radius ? Does the defined "speed" exceeds c, or what are the limits ?
Or generally, what observer (a) can see during collapse ?