Newton's Gravity & Lorentz Contraction: Is Modification Needed?

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Discussion Overview

The discussion revolves around the compatibility of Newton's gravity with the principles of special relativity, particularly focusing on whether modifications to Newton's gravitational law are necessary due to effects such as length contraction and the frame dependence of simultaneity.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants argue that Newton's gravity relies on the Euclidean distance between masses, which varies between different frames, suggesting a need for modification.
  • Others challenge the application of Newtonian gravity in relativistic contexts, emphasizing that gravity's instantaneous propagation contradicts relativistic principles.
  • A participant notes that simultaneity is frame-dependent, raising questions about how to apply Newton's law in moving frames.
  • Some contributions highlight that simply incorporating length contraction into Newtonian gravity does not adequately address the incompatibility with special relativity.
  • There are references to specific homework assignments that some participants find misleading or flawed in their approach to the problem.
  • One participant expresses curiosity about the failures of Newtonian mechanics within a special relativity framework, while another emphasizes that the fundamental incompatibility means one cannot derive correct answers using Newtonian gravity.

Areas of Agreement / Disagreement

Participants express conflicting views on whether length contraction alone is sufficient to necessitate modifications to Newton's gravity. While some assert that general relativity is required, others explore the nuances of how Newtonian mechanics fails in relativistic settings without reaching a consensus.

Contextual Notes

Limitations include unresolved definitions of simultaneity and the speed of observers, as well as the implications of instantaneous propagation in Newtonian gravity versus relativistic interactions.

Kashmir
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Newton's gravity depends on the euclidean distance between two masses.
Two comoving frames will have different values of length between masses so the forces will be different in two frames.
Is it enough to prove that the gravity rule has to be modified?
 
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That's a very misleading homework. If they had ask for the motion of a particle in the Coulomb field of a fixed (i.e., very massive) particle, neglecting radiation reaction, it'll have been fine, but to think one could use the Newtonian gravitational force in relativity is at least a bit questionable. One should rather ask for the solution of the geodesic worldline in the Newtonian approximation of the Schwarzschild spacetime, if one wants to discuss the motion of a planet around the Sun.
 
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PeroK said:
Here's an interesting homework assignment
I'm not sure I see how this thread is helpful. The thread left it hanging whether the answer given was correct (I don't think it is); in fact the thread left hanging a highly pertinent question from @Orodruin, namely, how ##\gamma## is to be defined, or more precisely how the speed ##v## is to be defined; is it the actually measured speed relative to static observers, or just the coordinate speed?

If there is a proof somewhere in the literature that, at least for some special cases, the heuristic "plug the Newtonian gravity formula into SR" happens to work, a reference to that might be helpful. I'm not sure any such reference exists. But certainly the thread referred to is not such a reference.
 
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Kashmir said:
Newton's gravity depends on the euclidean distance between two masses.
Two comoving frames will have different values of length between masses so the forces will be different in two frames.
Is it enough to prove that the gravity rule has to be modified?
There is a related question to this, namely, that Newton's gravity depends on the relative positions of the masses at some instant of time. But "instant of time", i.e., simultaneity, is frame dependent in relativity; if the two masses are moving relative to each other, their notions of simultaneity will be different, and which one should be used for the Newtonian force law? Is that enough to prove that the gravity rule has to be modified?

Einstein explicitly considered the latter question in 1907, and his answer was yes. I don't know if he explicitly considered whether the frame dependence of the distance itself would lead to a similar answer, but I think it would.
 
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Kashmir said:
Newton's gravity depends on the euclidean distance between two masses.
Two comoving frames will have different values of length between masses
PeterDonis said:
Newton's gravity depends on the relative positions of the masses at some instant of time. But "instant of time", i.e., simultaneity, is frame dependent in relativity
PeterDonis said:
Einstein explicitly considered the latter question in 1907
Actually, I think the question Einstein considered in 1907 was more basic than either of the above: Newtonian gravity says that gravity propagates instantaneously, but "instantaneously" is frame-dependent in relativity. A relativistic theory cannot have instantaneous propagation; instead, one would expect that a relativistic interaction would propagate at the speed of light, as electromagnetism does. But just plugging a speed of light interaction speed into Newtonian gravity does not work. Carlip's classic paper on aberration and the speed of gravity discusses this:

https://arxiv.org/abs/gr-qc/9909087
 
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PeterDonis said:
but I think it would.
You think its enough , this length contraction to decide that Newtons gravitation should be modified?
I am getting conflicting answers.
 
Kashmir said:
You think its enough , this length contraction to decide that Newtons gravitation should be modified?
I am getting conflicting answers.
Does it matter? You know the answer - that GR is needed - and in a sense that is the only answer. Asking whether length contraction by itself is enough is somewhat hypothetical.
 
  • #10
Kashmir said:
You think its enough , this length contraction to decide that Newtons gravitation should be modified?
Focusing on length contraction specifically is not really correct. Length contraction is not the only relevant consequence of SR that affects the Newtonian gravitation law, as I show in posts #6 and #7. So the correct question to ask is simply whether the Newtonian gravitation law can be incorporated as-is into a theory based on SR. And the answer to that question is no.
 
  • #11
Will this give you the right answer? No.
Will this give you an answer that is close? Sometimes.
Is it close enough? How could we possible tell you what "close enough" is?
 
  • #12
PeroK said:
That is not interesting. It is fundamentally flawed … as I pointed out in that thread …

vanhees71 said:
That's a very misleading homework. If they had ask for the motion of a particle in the Coulomb field of a fixed (i.e., very massive) particle, neglecting radiation reaction, it'll have been fine
As stated 😉
Orodruin said:
It is particularly unfortunate as you could actually make a reasonable problem by replacing gravity by the motion of a test charge in a static electric field.
 
  • #13
PeroK said:
Does it matter? You know the answer - that GR is needed - and in a sense that is the only answer. Asking whether length contraction by itself is enough is somewhat hypothetical.
I know that GR is needed, I was just curious and tried to see how many things went wrong with Newtonian mechanics in SR setting.
 
  • #14
Kashmir said:
I know that GR is needed, I was just curious and tried to see how many things went wrong with Newtonian mechanics in SR setting.
Newtonian mechanics and SR is pretty similar. There are equivalents of all three of Newton’s laws. The big difference being the structure of spacetime.

Newtonian gravity on the other hand is fundamentally incompatible with the spacetime structure of special relativity.
 
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  • #15
Kashmir said:
how many things went wrong with Newtonian mechanics in SR setting.
Just one. You get the wrong answer.

But isn't that enough?
 
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  • #16
Vanadium 50 said:
Just one. You get the wrong answer.

But isn't that enough?
You don't even get an answer as the two are incompatible.

This thread also reminded me of an XKCD classic:

1665671277965.png

With the alt-text: "Of these four forces, there's one we don't really understand." "Is it the weak force or the strong--" "It's gravity."
 
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