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Why does light fall?

  1. Apr 3, 2009 #1
    Light does gravitate --- there is plenty of sound evidence for this, such as gravitational lensing in astronomy. Gravity makes space refract, it seems.

    What theoretical explanation can be offered for this observation? The equivalence principle is often used, but invoking a principle smacks of avoiding something you don't really understand.

    Does special relativity require that light gravitates (because photons have measurable energy -- hence inertial mass -- and experiment shows that inertial masses gravitate) ? And if not, why not?
     
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  3. Apr 3, 2009 #2

    Xnn

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    Einstein's theory of special relativity does not address gravitation.

    On the other hand, the theory of general relativity does.
     
  4. Apr 3, 2009 #3
    Gravity makes space curved. Light travels in "straight" lines, where "straight" means "as straight as possible given the curvature of space itself". The curvature of a light beam is the curvature of the medium it passes through; it's not a property of the light beam.
     
  5. Apr 3, 2009 #4

    Wallace

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    I'm not sure I follow this line of reasoning. General Relativity stems entirely from a few foundations, including the equivalance principle. If you understand the equivalance principle then you understand why GR predicts gravitational lensing. If someone invokes the principle of inertia to explain why you need to apply the brakes on your car to stop moving (as opposed to just taking your foot of the accelerator) does this mean they don't understand why you need brakes? No, if you understand the principle of inertia you can invoke it to explain an example of its operation.
     
  6. Apr 3, 2009 #5

    Ich

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    You really got it backwards. The principle has not been invoked to explain a posteriori some experimental facts that would otherwise contradict the theory.
    GR is based on that principle, and GR predicts bending of light. It has been measured after the theory has been fully developed.
    On small scales the principle states that falling objects are free floating, with no forces acting on them. Thus they move just like in free space. You don't have to explain that light does nothing interesting if nothing acts on it.
    It's rather the ground that is accelerating upwards, that's why the "relative acceleration" (as measured in the ground system) is naturally independent of the properties of the free floating objects.
    The trick is to make this principle work on large scales also, that's where spacetime curvature comes into play.
     
  7. Apr 3, 2009 #6
    What's the equivalence principle?
     
  8. Apr 3, 2009 #7

    Wallace

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    In simple terms the equivalance principle states that an accelerated reference frame is equivalent to an un-accelerated reference frame in a gravitational field. Ich's post #5 gives some further exposition of this.

    The example given when I had GR lectures in grad school was to imagine you are in a box that you cannot see out of. You can do a bunch of experiments with pendulums, dropping balls etc and you infer that you must be simply sitting on the surface of the earth, since you measure a graviational acceleration of 9.8 m/s/s. But, think about the possibilty that you are instead in deep space (vaccum) and your box is being accelerated at a constant rate of 9.8 m/s/s by some kind of rocket. All of your experiments will give exactly the same result.

    Einsteins leap was to realise not that these two situations are indistinguishable, but rather than they are identical. As Ich suggested, if you imagine again you are sitting on the surface of the Earth, then in fact in the language of GR you are continually being accelerated upwards at 9.8 m/s/s by the force exerted by the surface of the Earth on your feet.

    In Newtonian physics we think of gravity as causing acceleration, but in GR in the language of the equivalence principle you are only 'accelerated' if your motion if altered by something other than gravity.

    Now, in relation to light, you can imagine in the rocket in space example, that if you have a small window that allows just a single beam of light into the side of your box, you will observe the path of the light to be curve. Hence by the equivalence principle we must see the same effect in the presence of a gravitationl field, hence we see gravitational lensing.
     
  9. Apr 3, 2009 #8

    George Jones

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    As usual, I don't have very much to say, and will only give a reference that might be relevant,

    http://arxiv.org/abs/gr-qc/9909014.

    Steve Carlip often does have interesting things to say.
     
  10. Apr 3, 2009 #9
    You're quite right, Xnn. Taken on its own, SR says nothing about gravity. But if you add in the results of Eotvos-type experiments, it can be used, as I summarised, to persuade people that light gravitates. Nice (but inaccurate?) for simple minded folk who don't appreciate the equivalence principle (EP) and all that goes with it. I guess that SR used this way will give answers out by a factor of 2, as Newtonian calculations do. Do you know if this is so?

    Thanks, Wallace, for this and your second post. But I'm afraid that my prejudice against principles (useful though they are) carries through to the inertia priniple as well. I don't really know what inertia is or what causes it. It's just a 'law' --- one that works pretty well, I must admit.

    I probably have got it backwards, as you say, or have put my thinking confusingly. But the fact that light gravitates is often introduced via the EP (e. g. by Rindler in section 1.21 of his Relativity and by Wallace in this thread (his post#7). I'm just suggesting that there is no need to rely on a principle (my prejudice) if one can offer a simpler rationale via something more readily understood, namely SR.

    Thanks for the reference, George. Carlip's section 3: General Covariance and the Weight of Light is indeed relevant to the guess I made when replying to Xnn above.
     
  11. Apr 3, 2009 #10

    Wallace

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    At the risk of getting overly philosophical, I think you are asking of empirical science something that it cannot provide. The best we can do is postulate principles and laws and then test them as rigourously as we are able. The only way we can ever 'explain' a principle or law is via a more fundamental principle or law, but then that principle is left 'unexplained'. I'm afraid I don't see how this infinite regression can be terminated by empirical science. Science is just a series of tested principles.

    There is a whole story we could get into about empiricism vs Artistotelean deductovism (sp?) but it's been a long time since studied the details and I normally only bang on about this kind of stuff after a few beers.
     
  12. Apr 3, 2009 #11
    Light falls and gains energy in a gravatational field as shown by Pound and Rebka in their famous Mossbauer Effect experiment with iron-57 about 1959.
     
  13. Apr 3, 2009 #12
    For me, the danb's answer in Post # 3 is just fine. Of course you can, as usual, keeping asking "why" and quickly get to unanswerables....yet I think general relativity is about as good a theory as is available.

    On the other hand, it could be argued that the "theoretical explanation" depends on which model you'd prefer to use....particle, electromagnetic wave, quantum, etc...then the answer might be framed different ways. It would be interesting to reconcile them.

    In Post #9, Oldman expresses displeasure with certain laws and principles and while I understand that (because we may not know why they work) feeling, that's really true of most of physics...if math predicts and measurement confirms, then we have a tool even though we might not understand exactly why....even if we start as Einstein did with an equivalence principle, we may never know exactly why it works....it's just a good guess....

    And since nobody really knows what light nor gravity is, asking why one effects the other may be futile for the purist...
     
  14. Apr 4, 2009 #13

    atyy

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    Special relativity does not require that light gravitates, because it is possible to make a relativistic theory of gravity in which the trace of the energy tensor (instead of the energy tensor itself) is gravitational mass. The trace of the energy tensor of light is zero, so light would not gravitate. However I don't know if the equivalence principle requires that light gravitates, since this alternative relativistic theory also satisfies some form of the equivalence principle. See the comments on Nordstrom's second theory:
    http://www.einstein-online.info/en/spotlights/equivalence_deflection/index.html [Broken]
    http://arxiv.org/abs/gr-qc/0405030
    http://arxiv.org/abs/gr-qc/0611100
     
    Last edited by a moderator: May 4, 2017
  15. Apr 5, 2009 #14
    I agree with all you say here, and don't want to get philosophical. I remember that Henry Ford said that "History is bunk" and can only wonder if he had more pungent views on philosophy which I could also agree with. And I regret that this kind of communication can't involve sharing a few beers.

    Yes, I agree here too. But I do prefer explanations based as far as possible on observation, that delay for as long as possible getting down to the level of principles, which I feel have an ex cathedra flavour.

    As far as light falling (which one cannot doubt, as Bob S points out) and the fact that there are good reasons why:
    I still don't understand why it is so wrong to reason, for introductory purposes only?, that light falls "because photons have measurable energy -- hence inertial mass -- and experiment shows that inertial masses gravitate". All good observational stuff far removed from philosophy and the history of Nordstrom's theories. But perhaps I'm just too simple-minded.
     
  16. Apr 5, 2009 #15

    JesseM

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    There's no logical connection between the idea that light gravitates and the idea that it falls in the presence of an external source of gravity (after all, the rate at which an object falls in an external field is totally independent of its own mass, and thus independent of its own gravitational pull). It's also not clear what you mean by "inertial mass" here--if you mean "rest mass" you're incorrect, since something with zero rest mass but nonzero momentum can have nonzero energy in relativity.
     
  17. Apr 5, 2009 #16

    JesseM

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    See http://www.aei.mpg.de/einsteinOnline/en/spotlights/equivalence_principle/index.html [Broken] for a good overview.
     
    Last edited by a moderator: May 4, 2017
  18. Apr 5, 2009 #17

    atyy

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    That light should fall because it has energy, and energy has mass is certainly a useful heuristic. However, it is only a heuristic, and not a requirement.

    Edit: Your argument about the universality of free fall is an EP argument. Redshift and local light bending are required by the EP, global light bending is not required, that light should curve space is also not required.
     
    Last edited: Apr 5, 2009
  19. Apr 5, 2009 #18
    Thanks for pointing this out, atyy--here, and in a previous post. From a rather good source, and paraphrased, "it's difficult to conceive of a situation where the Newtonian equivalence principle is not equivalent to the Einstein equivalence principle." But just about anything with a stress energy tensor unlike common matter is a possible candidate to violate both.
     
  20. Apr 5, 2009 #19
    The real question is, "Why does the surface of a massive body accelerate outward?" or "Why does earth's surface accelerate upward?"

    It's easily observed that earth's surface accelerates upward with respect to any unaccelerated object (freefall) at the rate of 9.8 m/s^2, and we of course "feel" the force of this acceleration against our feet when we stand. It should be no surprise that we would see the path of a light ray "bend" relative to an accelerating reference frame, just like it would relative to an accelerating spacecraft.
     
  21. Apr 5, 2009 #20
    And what would some dark energy do in the presence of some outwardly accelerating body. Would it be carried along? Would it accelerate outwardly faster than the Eath's surface?
     
    Last edited: Apr 5, 2009
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