Bending of Light: General Relativity Explained

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Discussion Overview

The discussion revolves around the bending of light as explained by general relativity, specifically addressing whether this phenomenon is due to the curvature of spacetime caused by massive objects or if it arises from other properties of acceleration. Participants explore the implications of acceleration in both flat and curved spacetime and the distinction between geometric effects and coordinate artifacts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that spacetime curvature due to massive objects leads to the deflection of light, while others clarify that light can bend in accelerated coordinates without a force acting on it.
  • There is a discussion about whether the curvature observed during acceleration is a result of spacetime curvature or a property of acceleration itself, with some arguing that bending can occur in flat spacetime.
  • One participant emphasizes that the bending of light due to curved spacetime is a geometric phenomenon and should not be conflated with the effects of acceleration, which can be described using different coordinate systems.
  • Another point raised is the equivalence principle, which suggests that the effects of acceleration and gravitational fields are indistinguishable under certain conditions, leading to further exploration of mass and energy density as causes of curvature.
  • Participants discuss the geometric meaning of acceleration as measured by an accelerometer, distinguishing between absolute curvature of an observer's worldline and the coordinate-dependent trajectory representation.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between acceleration and spacetime curvature, with no consensus reached on whether acceleration inherently implies curvature or if they are distinct phenomena. The discussion remains unresolved regarding the implications of these concepts.

Contextual Notes

Participants note that the bending of light and the effects of acceleration can be interpreted differently depending on the chosen coordinate system, highlighting the complexity and nuance in understanding these concepts within general relativity.

shounakbhatta
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Hello All,

Kindly apologize if this question sounds rudimentary.

General relativity which shows the bending of light. Is it due to:

(a) Spacetime is curved due to massive objects and when light passes through that object, facing the obstruction it bends?

(b) There is as such no force which causes the photon to bend?

Am I right?
 
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I think you're nearly right. Perhaps

a) Spacetime is curved due to massive objects and when light passes near that object it is deflected.

is more accurate. There is no force.

Light bends in accelerated coordinates also, see http://www.Newtonphysics.on.ca/einstein/chapter10.html
 
Thank you.

One small question. When we are accelerating, we get a curve. Is it due to the curvature of spacetime or any specific property of acceleration?
 
shounakbhatta said:
One small question. When we are accelerating, we get a curve. Is it due to the curvature of spacetime or any specific property of acceleration?
Acceleration is a vector so it has direction and magnitude and no other properties. The bending of light due to acceleration (say in the 'Einstein elevator' ) can happen in flat spacetime, so it cannot be attributed to spacetime curvature.

I've attached a paper by Ehlers and Rindler which may be helpful.
 

Attachments

shounakbhatta said:
One small question. When we are accelerating, we get a curve. Is it due to the curvature of spacetime or any specific property of acceleration?

Don't confuse these two things. The deflection of light due to curved space-time geometry is an honest geometric effect and it doesn't disturb the fact that a null geodesic is describing this light ray; trajectories of observers and light rays being curved in different coordinate systems is a coordinate artifact. In the end light rays (within the geometrical optics approximation) always get described by null geodesics in the absence of non-gravitational interactions and that's what counts.
 
So, can we say that when we are accelerating in even a flat spacetime, we get a curve?

Also, bending of light due to curved spacetime is a geometric phenomena and these two are different and should not be confused.

Mass causes the curvature and gravity is the geometric phenomena of curvature. Right?
 
shounakbhatta said:
So, can we say that when we are accelerating in even a flat spacetime, we get a curve?

Also, bending of light due to curved spacetime is a geometric phenomena and these two are different and should not be confused.


The equivalence principle states that the effect of acceleration cannot be distinguished from the effect of a gravitational field, with provisos about the extent of the experiment and the 'uniformity' of the field.

Mass causes the curvature and gravity is the geometric phenomena of curvature. Right?
Mass and energy density cause curvature.
 
shounakbhatta said:
So, can we say that when we are accelerating in even a flat spacetime, we get a curve?

Let me clarify something. If an observer is accelerating (flat space-time, curved space-time doesn't matter for what's to come) then this observer can measure this acceleration locally using an accelerometer. Geometrically, the worldline of the observer has a path curvature in space-time given by the 4-acceleration. This is an absolute measure of curvature of the worldline that has no dependence whatsoever on a choice of coordinate system (hence why it is a geometrically meaningful quantity). This goes back to the fact that the observer himself can measure the acceleration using an accelerometer.

On the other hand, we can choose a particular set of coordinates and write down the coordinate trajectory of the observer. This will give in general a curved trajectory for the observer in these coordinates and hence has no geometric meaning; it is simply the trajectory of the observer as represented in this specific choice of coordinates. I can just as easily go to a coordinate system that is comoving with the observer and in this set of coordinates the observer is always at a constant spatial coordinate and hence just has a straight line trajectory along the temporal axis.
shounakbhatta said:
Also, bending of light due to curved spacetime is a geometric phenomena and these two are different and should not be confused.

Mass causes the curvature and gravity is the geometric phenomena of curvature. Right?

Yep.
 
Last edited:
Thanks.

Ok, actually I was getting confused that acceleration causes a curve so it gives a hint that spacetime must be curved. Thank you for clearing the doubt.
 

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