Light Behaviour: Does Gravity Accelerate Light?

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Discussion Overview

The discussion revolves around the question of whether gravity accelerates light, particularly in the context of general relativity and the bending of light by massive bodies. Participants explore the implications of light following geodesics in curved spacetime, the semantics of acceleration, and the effects of gravitational redshift and blueshift.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants argue that light follows a straight path in its own frame of reference, suggesting that gravity bends spacetime rather than accelerating light.
  • Others propose that the change in the apparent direction of light could be interpreted as a change in velocity, which implies acceleration.
  • A participant raises the semantic issue of defining "acceleration" in the context of light, preferring to describe light as traveling along a geodesic.
  • There is mention of the gravitational redshift and blueshift, with some participants questioning whether these effects could be seen as light being accelerated or decelerated.
  • One participant references the Harvard tower experiment, noting that the measured blue shift of light falling downwards aligns with the energy gain expected from a massive body falling, prompting questions about whether this supports special or general relativity.
  • Another participant discusses the contributions of coordinate acceleration and spacetime curvature to the deflection of light, indicating that both factors play a role in the observed phenomena.

Areas of Agreement / Disagreement

Participants express differing views on whether gravity can be said to accelerate light, with no consensus reached. Some emphasize the role of spacetime curvature while others focus on the implications of light's behavior in gravitational fields.

Contextual Notes

Participants note the complexities involved in defining acceleration for light and the limitations of applying traditional concepts of acceleration to massless particles. The discussion also touches on the historical context of Einstein's calculations regarding light deflection.

Nuclear on the Rocks
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Hello! I am somewhat a layman, but i have a question.When we talk of bodies with large gravities bending light, are they accelerating it?
 
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No, if I understand the situation properly. The light is still following what to it is a straight line, so there is no acceleration imparted to it. Gravity bends the space itself, but the light has no way of 'knowing' that.
 
The Speed remains constant, but the apparent direction changes, therefore this is a change in velocity which implies an acceleration.
 
I think much of the question is a matter of semantics - what does one mean by "accelerating" the light?

I think that I generally prefer the explanation that light travels along a geodesic, though, for the following reason. If we say that light "accelerates", how do we assign a number to this acceleration to quanfity it?

We can talk about the proper acceleration of physical objects by looking at the 4-acceleration, but I don't see how to make this approach work for light. (For instance, if we try to take the limit of a 4-velocity of a massive object as it approaches c - it doesn't have a limit, so we don't even have a 4-velocity for light, much less a 4-acceleration).

Maybe there is some way around this difficulty, but I don't know what it is, and I don't recall reading anything on the topic. It might be possible to replace proper time with some affine parameter, for instance. So on the whole, I'd rather stick with saying that light follows a geodesic, it seems the simplest approach.
 
What some call "bending of light" is simply an effect of the curvature of spacetime (e.g geodesic convergence and divergence). In general relativity a photon in a gravitational field obviously does not accelerate for it would completely invalidate the foundations of the theory.

Pervect said:
It might be possible to replace proper time with some affine parameter, for instance.
Of course that is possible. But then one ought to explain the physical meaning of that parameterization as well, otherwise it is justs playing mathematics with GR.
 
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Isn't the gravitational red/blue shift rather like the light having been 'accelerated' or 'decelerated' ?

Question - if light reaches me from a source accelerating away from me, is there a frequency shift component for instantaneous velocity, and a separate contribution from the acceleration ?

I suppose I should go and look again at the Rindler space-time.
 
Mentz114 said:
Isn't the gravitational red/blue shift rather like the light having been 'accelerated' or 'decelerated' ?
What is called gravitational red- and blueshift of photons are the effects of the curvature of spacetime. The photon itself undergoes no changes whatsoever.

The curvature of spacetime determines the ratio between the emitter's and absorber's measurement of the frequency of a photon.

Mentz114 said:
I suppose I should go and look again at the Rindler space-time.
The Ridler chart is very interesting but notice that Minkowski spacetime only deals with the kinematics of acceleration. A more complete understanding of acceleration can only be obtained in general relativity, where the kinematics, if we even can speak of kinematics here, is simply a reflection of the dynamics.

Afterall: In the general theory of relativity the doctrine of space and time, or kinematics, no longer figures as a fundamental independent of the rest of physics. The geometrical behaviour of bodies and the motion of clocks rather depend on gravitational fields which in their turn are produced by matter.
 
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Looking at it from a semi-classical standpoint. Could you think of it like this?

E(photon) = p*c .. So gravity imparts a force based off of this photon's relativistic momentum. The gravitation force of course being something along the lines of centripetal force (i.e acceleration perpindicular to the direction of motion of the photon).
 
What is called gravitational red- and blueshift of photons are the effects of the curvature of spacetime. The photon itself undergoes no changes whatsoever.

MJ, this puzzles me. In the Harvard tower experiment, light was beamed downwards i.e. it 'fell', and the blue shift was very precisely measured.
The gain in the light energy due to the blue shift was calculated to be exactly ( within the exp. error) the amount that a massive body would have gained by falling. They did it the other way around also and got the same agreement.

Was this a test of SR or GR ?

The experiment was by Pound and Snider in 1965.

A description is here -
http://www.mth.uct.ac.za/omei/gr/chap5/node2.html
 
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  • #10
Mentz114 said:
MJ, this puzzles me. In the Chicago tower experiment, light was beamed downwards i.e. it 'fell', and the blue shift was very precisely measured.
The gain in the light energy due to the blue shift was calculated to be exactly ( within the exp. error) the amount that a massive body would have gained by falling. They did it the other way around also and got the same agreement.

Was this a test of SR or GR ?

Well if you say Massive Body, I would think GR.
 
  • #11
MeJennifer said:
What some call "bending of light" is simply an effect of the curvature of spacetime (e.g geodesic convergence and divergence). In general relativity a photon in a gravitational field obviously does not accelerate for it would completely invalidate the foundations of the theory.
Actually 1/2 the value of the deflection is due to coordinate acceleration while the other 1/2 is due to spacetime curvature.

Pete
 
  • #12
pmb_phy said:
Actually 1/2 the value of the deflection is due to coordinate acceleration while the other 1/2 is due to spacetime curvature.
Well that is true, that 1/2 is actually due to the principle of equivalence alone while the other 1/2 is due to the curvature of spacetime.
Note that the first 1/2 applies to all metric theories.

Einstein was initially wrong in his calculations, he only took the equivalence principle in consideration, and so he calculated the first half only. Later he corrected it and included the curvature part as well.
 
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