Parallel transport to explain motion of light near black hole?

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The discussion revolves around the application of parallel transport in explaining the behavior of light near black holes. The instructor is exploring whether parallel transport can clarify how the speed of light appears altered to distant observers, particularly in the context of gravitational effects. While parallel transport preserves the lightlike nature of a vector, it does not directly account for changes in the observed speed of light, which is more related to gravitational redshift and coordinate effects. The conversation also touches on the distinction between physical and coordinate speeds, emphasizing that proper speeds are more significant in gravitational contexts. Ultimately, the instructor seeks to refine their teaching approach to effectively convey these complex concepts to non-science majors.
  • #31
martinbn said:
If you parallel transport a vector around a loop you can end up with a vector with a diffrent orientation. Then why can't you end up with a vector at 180 degrees angle with the original i.e. a scalor multiple, where the scalor is -1? It seems quit possible. Start at the north pole facing south, walk along a meridian till you reach the equator, move along the equator for half of the circumference, then go back north to the pole. You end up facing the other way compare to you start.

You're right, that's a clear counterexample. I think the problem is my assertion that the result generalizes from infinitesimal parallelograms to larger paths. Now that I think more carefully about it, it's clearly wrong. If you add a bunch of vectors that are not parallel to a given line, you can still get a sum that's parallel to the line.
 
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  • #32
After posting a bunch of wrong stuff about the rescaling of null vectors, I think I finally understand it better. The antisymmetry of the Riemann tensor on its first two indices is exactly the condition needed so that parallel transport around an infinitesimal closed loop doesn't change inner products. For such a loop lying in a fixed plane, the set of possible actions by Riemann tensors are therefore the six-dimensional set of linear transformations that preserve inner products. In other words, they are the set of possible Lorentz transformations. Such a transformation can certainly take a null vector and rescale it.
 
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