Equation for path of light in GR

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Discussion Overview

The discussion revolves around the path of light in the context of General Relativity (GR), particularly focusing on the implications of treating light as a particle in a Newtonian framework and the accuracy of such approaches in predicting light bending near gravitational fields, such as those around black holes.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants discuss the derivation of black hole radius using Newtonian escape velocity and question whether this approach yields correct geodesics or is merely an approximation.
  • One participant asserts that due to the equivalence principle, correct geodesics can be obtained using equations for light bending in an accelerating spaceship, while another counters that the full theory predicts twice the light bending compared to this calculation.
  • There is a claim that one cannot make statements about the path of a single photon, as it is said to take "all possible paths," and that in GR, light travels at speed c without a defined distance between emission and absorption.
  • Another participant emphasizes that discussions about null geodesics in gravitational fields pertain to classical beams of light rather than quantum mechanics, noting that photons travel in straight lines despite the "all possible paths" concept being relevant for interference effects over short distances.
  • Questions arise regarding the exactness of the prediction of twice the light bending, with references to the weak equivalence principle and local experiments.

Areas of Agreement / Disagreement

Participants express differing views on the validity of using Newtonian analogies for light bending, the implications of the equivalence principle, and the nature of photon paths. There is no consensus on the accuracy of the approximations discussed or the interpretation of light behavior in gravitational fields.

Contextual Notes

Participants highlight limitations in understanding the path of light, particularly regarding the assumptions made about photon behavior and the conditions under which certain approximations hold true. The discussion also touches on the distinction between classical and quantum descriptions of light.

dsoodak
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In several places I've seen a derivation of the radius of a black hole by simply determining when the Newtonian escape velocity will reach c. Similar analogies are commonly used to explain light being bent by a gravitational field.

So will treating light as a particle traveling at speed c in a Newtonian universe actually give correct geodesics or is this just a +/- order of magnitude approximation only useful for explaining the concepts without going into tensor calculus?

Dustin
 
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dsoodak said:
or is this just a +/- order of magnitude approximation only useful for explaining the concepts without going into tensor calculus?

Yes.
 
OK.

But I assume that due to the equivalence of gravitational and linear acceleration, you CAN obtain correct geodesics if you use the equations for apparent bending of light inside a spaceship whose acceleration is the same as that in the local gravitational field.
 
dsoodak said:
OK.

But I assume that due to the equivalence of gravitational and linear acceleration, you CAN obtain correct geodesics if you use the equations for apparent bending of light inside a spaceship whose acceleration is the same as that in the local gravitational field.

No. The full theory predicts twice the light bending you'd get from this calculation. To get the path of light, you need to solve the geodesics. Which isn't terribly hard for the case of light, just remember that the Lorentz interval is zero,.
 
pervect said:
No. The full theory predicts twice the light bending you'd get from this calculation. To get the path of light, you need to solve the geodesics. Which isn't terribly hard for the case of light, just remember that the Lorentz interval is zero,.
AFAIK, this is for the Schwarzschild spacetime, I think that he is correct for a rocket accelerating in flat spacetime.
 
i was always taught that you cannot say anything about a photon in between the time it is emitted and the time it is absorbed. a photon takes "all possible paths". in GR, light travels at C - where there is no definition of either time or distance, ie, for the photon, there is no distance between the place where it is emitted and the place where it is absorbed. i do not think you can make any kind of statement about the path of a single photon.
 
pervect said:
No. The full theory predicts twice the light bending you'd get from this calculation.

I meant the example to be only over short distances (so direction of gravitational "force" doesn't change much) in a case where tidal forces are minimal.
According to the "weak equivalence principle", any experiments performed locally should be indistinguishable from the accelerated spacecraft , right?

Also: does it actually come to exactly twice the light bending, or is this just an approximation?
 
i was always taught that you cannot say anything about a photon in between the time it is emitted and the time it is absorbed. a photon takes "all possible paths". in GR, light travels at C - where there is no definition of either time or distance, ie, for the photon, there is no distance between the place where it is emitted and the place where it is absorbed. i do not think you can make any kind of statement about the path of a single photon.
People have fallen into the unfortunate habit of saying "photon" when what they really mean is light ray. When we talk about null geodesics in a gravitational field, we mean the propagation of a classical beam of light - nothing quantum mechanical involved.

Quantum mechanics is appropriate in limited situations. E.g. when the light intensity is very low, a continuous light ray is resolved into individual photons. Experiments that fire lasers at retroreflectors on the surface of the moon receive back only a few photons. But did you notice something about this? even photons travel in a straight line. The photons don't zigzag around "all possible paths", they always come back right from the direction of the retroreflector! That's because in addition to the low intensity you have to ask about the wavelength. "All possible paths" is relevant for interference effects, and this matters only over short distances, the same distance scale as a wavelength.

For the path of a light ray in the gravitational field of a black hole, you'd need to worry about this only if the wavelength of the light was very long, comparable to the size of the hole.
 
dsoodak said:
I meant the example to be only over short distances (so direction of gravitational "force" doesn't change much) in a case where tidal forces are minimal.
According to the "weak equivalence principle", any experiments performed locally should be indistinguishable from the accelerated spacecraft , right?

Also: does it actually come to exactly twice the light bending, or is this just an approximation?
I guess so... and It is exactly twice:

http://www.mathpages.com/rr/s6-03/6-03.htm

(but I'm sure that there was a page with a graph... )
 
  • #10
thanks for the link!
 

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