yuiop said:
The local velocity of a free falling object as measured by a stationary observer at r for an object that is initially at rest and released from infinity is:
v= c \sqrt{\frac{Rs}{r}}
For an observer very close to the event horizon so that r is nearly equal to Rs, the local velocity approaches c. The catch is that we can not have an observer exactly at the event horizon (r=Rs) so the velocity is never exactly c but we can take the observer as close as we like to the event horizon and the maximum velocity to as close as we like to c as long as the difference we are satisfied with is not exactly zero.
I fully agree with yuiop here.
Since you asked about the coordinate velocity falling from infinity I will add this here.
The formula is:
<br />
\sqrt { \left( 1- \left( 1-{{\it v0}}^{2} \right) \left( 1-{\frac {{<br />
\it rs}}{r}} \right) \right) \left( 1-{\frac {{\it rs}}{r}} \right) <br />
^{2}}<br />
v0 is the initial speed at infinity, rs is the Schwarzschild radius.
The coordinate velocity does not have a maximum but this is a good opportunity to address a misunderstanding that many people have. A gravitational field does not necessarily accelerate an object towards the center of gravity. In fact above a certain velocity gravitation decelerates it, by the way, just like in the case of light.
See the attached graph for the coordinate velocity of 3 different scenarios (initial velocity=0, 1/sqrt(2) and 1/sqrt(3) ), you can see what I am saying.
Now you mention that the object in question has mass, for simplicity I assume you mean that in that case the object does not have to travel at c (by the way the formula I wrote above also works for c). If not then the problem becomes a lot more complex. Is that what you want to discuss?
skeptic2 said:
What is the velocity profile of a free falling object inside the event horizon?
For coordinate velocity it is the same formula, I added a graph for that case as well (initial velocity=0, 1/sqrt(2) and 1/sqrt(3) ). You can determine it all the way up to, but not including R=0.
In addition we can also calculate the proper velocity (d proper length/d tau), a third graph (initial velocity=0, 1/sqrt(2) and 1/sqrt(3) ) will show this relationship, the formula is:
<br />
\sqrt {1- \left( 1-{{\it v0}}^{2} \right) \left( 1-{\frac {{\it rs}}{<br />
r}} \right) }<br />