The speed of gravitational field propagation

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Discussion Overview

The discussion centers on the speed of gravitational field propagation, particularly within the frameworks of special and general relativity. Participants explore whether gravity must propagate at the speed of light and consider alternative speeds, as well as implications for orbital stability in celestial mechanics.

Discussion Character

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

Main Points Raised

  • One participant questions if it is theoretically valid for gravitational fields to propagate at speeds less than the speed of light, such as 0.9c or 0.99c.
  • Another participant expresses confusion about how planets maintain stable orbits given the time delay in gravitational influence from the sun.
  • Some participants reference an article discussing how certain effects of gravity may compensate for propagation delays, but express skepticism about the explanations provided.
  • A participant critiques the argument that gravitational equations inherently cancel out retardation effects, suggesting it lacks depth and may be oversimplified.
  • There is mention of the quadrupole dependence of gravity and how it relates to gravitational radiation, with some participants seeking clarification on the technical aspects of these concepts.
  • Concerns are raised about the implications of gravitational propagation speed on orbital stability, with references to the non-centrality of forces in general relativity.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the speed of gravitational propagation or the implications for gravitational theory. Multiple competing views and uncertainties remain regarding the necessity of gravity propagating at the speed of light and the effects of propagation delay on orbital stability.

Contextual Notes

Some participants note the limitations of existing explanations, particularly regarding the mathematical underpinnings of gravitational effects and the assumptions made in various theories. There is also a recognition that the discussion involves complex technical details that may not be fully addressed.

blaksheep423
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I am working on some interesting topics which relate to the speed at which gravity propagates. My question is this: within the frameworks of special and general relativity (or any other widely accepted theory, for that matter), is it necessary for gravitons/gravity waves to propagate at exactly the speed of light? Is it theoretically valid to suppose that gravitational fields could propagate at speeds of 0.9c, or 0.99c, etc.?

The limited amount of online research I've done concerning this has told me that, using a binary star system, the speed of gravity has been experimentally measured to within 0.95c, which, when coupled with a 0.25 experimental error, led to the assumption that gravity propagates at exactly c. Is there any theoretical work or research which refutes this, or any other reason to intelligently doubt it?

Thank you in advance for your time and your responses
 
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I always kind of wondered how planets could keep a stable orbit around the sun while the suns gravity takes 500 seconds to reach the Earth and the sun goes around the milky way at 486,000 miles per hour, i would figure that delay would stop things from orbiting but what do i know.
 
rathat said:
I always kind of wondered how planets could keep a stable orbit around the sun while the suns gravity takes 500 seconds to reach the Earth and the sun goes around the milky way at 486,000 miles per hour, i would figure that delay would stop things from orbiting but what do i know.
There's a good discussion of how certain effects of gravity "compensate" for the propagation delay here:

http://math.ucr.edu/home/baez/physics/Relativity/GR/grav_speed.html
 
wow, that can't be a more perfect article on my question.
 
this article sums up what i already knew, but is there any indication that the speed of gravity may not be exactly c? and is it absolutely essential to any standing theory that gravity propagate at the speed of light, or is it conceiveable that it could be slightly less?
 
JesseM said:
There's a good discussion of how certain effects of gravity "compensate" for the propagation delay here:

http://math.ucr.edu/home/baez/physics/Relativity/GR/grav_speed.html


Jesse; thanks for the link.
I've seen this argument many times in attempts to resolve the issue of grav. propagation delay causing orbital instability ...

I appreciate Carlip, et al, and their Gen Rel. point of view claiming that the speed of gravity explanation is analogous to Electrodynamic equations, but simply saying "when you solve the gravitational eqns. ...a cancellation of retardation effects occur" really seems like handwaving. Van Flandern and others do bring up some valid counter points... (PLEASE, folks; no flaming about Van Flandern...that is NOT the point here.)

It would be nice if a little more in depth analysis could clear up a few questions which I find Carlip has not addressed...
So let me start by asking you, Jesse, since I see you to be exacting in many of your responses.
If you don't feel you have a handle on this issue I understand...but I'm NOT looking for another link to Carlip Vs. Van Flandern debate.. (I've read all the counter punches and am not satisfied. :smile: )


First, let me say I agree with GR in most of its predictions, and I think Carlip tries to get to the real point by admitting , " Strictly speaking, gravity is not a "force" in general relativity,..." And I think he should have left it there. So there would be no need to address the non-centrality of forces...which causes the orbital instability problem.

But since he continues (in the weak field approx.), "one finds that the "force" in GR is not quite central--it does not point directly towards the source of the gravitational field--and that it depends on velocity as well as position. The net result is that the effect of propagation delay is almost exactly cancelled..."

Again apparent handwaving...

First, let me ask you....Is not this "velocity dependent" force in Gen Rel. based upon a v^2 term, namely v^2/c^2 ??

BTW, please give me simple answers WITHOUT using latex since all latex stuff is blacked out on my computer ( maybe that's asking a lot , but try me). also, I post rather infrequently, and so it may be some time before I respond...so please be patient).

Thanks.
:smile:
 
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Creator said:
I appreciate Carlip, et al, and their Gen Rel. point of view claiming that the speed of gravity explanation is analogous to Electrodynamic equations, but simply saying "when you solve the gravitational eqns. ...a cancellation of retardation effects occur" really seems like handwaving.
Why do you think it is handwaving? Presumably there are technical details behind that statement, which was just a nonmathematical one for an article aimed at a general audience.
Creator said:
So let me start by asking you, Jesse, since I see you to be exacting in many of your responses.
If you don't feel you have a handle on this issue I understand...but I'm NOT looking for another link to Carlip Vs. Van Flandern debate.. (I've read all the counter punches and am not satisfied. :smile: )
I am not very well-versed in the technical details of GR, so I can't help you with that. Perhaps someone else here can answer your questions. In the meantime you may find at least some useful info on these earlier physicsforums threads discussing the quadrupole dependence of gravity:

https://www.physicsforums.com/showthread.php?t=148954
https://www.physicsforums.com/showthread.php?t=147047
https://www.physicsforums.com/showthread.php?t=145020

Creator said:
First, let me say I agree with GR in most of its predictions, and I think Carlip tries to get to the real point by admitting , " Strictly speaking, gravity is not a "force" in general relativity,..." And I think he should have left it there. So there would be no need to address the non-centrality of forces...which causes the orbital instability problem.
Just because it's not a force doesn't mean we don't still need to explain why there is no orbital instability problem. GR is still after all a local theory--I'm pretty sure it would be true for example that the curvature of spacetime in a given region is determined only by points in the past light cone of that region, so for example if the Sun were split into pieces which went in different directions at nearly the speed of light, this couldn't have an effect on the orbits of the planets until the event of the splitting entered their past light cones.
Creator said:
But since he continues (in the weak field approx.), "one finds that the "force" in GR is not quite central--it does not point directly towards the source of the gravitational field--and that it depends on velocity as well as position. The net result is that the effect of propagation delay is almost exactly cancelled..."

Again apparent handwaving...
Do you really imagine there is no math behind it to make it precise?
Creator said:
First, let me ask you....Is not this "velocity dependent" force in Gen Rel. based upon a v^2 term, namely v^2/c^2 ??
Did you read this somewhere, or conclude it from some equation, or what? According to the threads I quoted earlier it sounds a bit more complicated, post #1 on this thread says "the strongest type of gravitational radiation from an isolated concentration of mass-energy occurs when the quadrupole moment tensor of the source of the field has a nonzero second derivative", and post #13 on this one adds: "Properly speaking, there can be other sources of gravitational radiation in addition to the quadrupole mass moment. For example, a source with constant quadrupole mass moment but time varying octupole mass moment will radiate, but this "octupole radiation" is far weaker than quadrupole radiation. And in addition to quadrupole mass moment there is a current quadrupole moment."
 
Jesse; thanks for your respnse but you are missing the point of my post entirely.
Carlip's answer is not about gravitational WAVES, i.e., quadrupolar gravitational radiation. Please read it again.


JesseM said:
I am not very well-versed in the technical details of GR, so I can't help you with that. Perhaps someone else here can answer your questions.

Thanks for admitting it.
Anyone else who is familiar with the 'speed of gravity' arguments want to give it a try?...again...the question is...

In Carlip's response as to how GR explains why the speed of gravity itself can have propagation delay without causing orbital instability , he says: "the 'force' in GR... depends on velocity as well as position. The net result is that the effect of propagation delay is almost exactly cancelled..."

This apparent handwaving cannot be denied without more thorough examination.

My first question is: Does not this velocity dependent "force" in GR actually depend upon a v^2 term, or more precisely, upon v^2/c^2 ??

Anyone?
 
simply saying "when you solve the gravitational eqns. ...a cancellation of retardation effects occur" really seems like handwaving.
Yeah, and saying that Carlip is "simply saying..." really seems like distorting the truth.

Carlip's answer is not about gravitational WAVES, i.e., quadrupolar gravitational radiation.
It is about gravitational waves also; please read it again.

Does not this velocity dependent "force" in GR actually depend upon a v^2 term, or more precisely, upon v^2/c^2 ??
Yes.

Carlip presents a rigorous derivation which is hard to follow, of course. Therefore, additionally, he presents a less involved mathematical and physical argumentation from "first principles". To make sure that everybody understands, he also describes his findigs in plain English. What more could he do?

Accusing him of handwaving seems quite dishonest to me, as you surely must know the difference between "I don't understand his derivation" and "he gives no derivation".
 
  • #10
Creator said:
Jesse; thanks for your respnse but you are missing the point of my post entirely.
Carlip's answer is not about gravitational WAVES, i.e., quadrupolar gravitational radiation. Please read it again.
Many of his comments are about gravitational waves. But I think I understand, your question is more about the "compensating effects" that occur even in situations where gravitational waves are not being emitted, correct?
Creator said:
In Carlip's response as to how GR explains why the speed of gravity itself can have propagation delay without causing orbital instability , he says: "the 'force' in GR... depends on velocity as well as position. The net result is that the effect of propagation delay is almost exactly cancelled..."

This apparent handwaving cannot be denied without more thorough examination.

My first question is: Does not this velocity dependent "force" in GR actually depend upon a v^2 term, or more precisely, upon v^2/c^2 ??
Can you explain where specifically you get the idea that it depends on a v^2 term? I think it would help others to address your question. Again, have you seen this stated somewhere, are you deriving it from some equation, or what?

Also, I got the idea that when he said the force "depends on velocity as well as position", he meant that in the weak-field approximation, the gravitational force an object A feels from another object B which lies X light-seconds away is not directed at the position B was X seconds ago, but rather is directed towards where the object B would be if we took its velocity vector X seconds ago and used it to "extrapolate" its current position under the assumption it had moved at constant velocity for the last X seconds. So the force would be directed towards the actual present position of B if it had indeed moved at constant velocity, whereas if B was accelerated during the last X seconds than this wouldn't have any effect on A until a wave created by the acceleration reached A, until then A would continue to be pulled towards the position of an imaginary phantom version of B that had not accelerated. This would fit with what Carlip said about electromagnetism:
This cancellation may seem less strange if one notes that a similar effect occurs in electromagnetism. If a charged particle is moving at a constant velocity, it exerts a force that points toward its present position, not its retarded position, even though electromagnetic interactions certainly move at the speed of light. Here, as in general relativity, subtleties in the nature of the interaction "conspire" to disguise the effect of propagation delay. It should be emphasized that in both electromagnetism and general relativity, this effect is not put in ad hoc but comes out of the equations. Also, the cancellation is nearly exact only for constant velocities.
Am I incorrect in my understanding of what Carlip said? If my understanding is right, then what would be the corresponding physical meaning of your statement that the force depends on a "v^2 term"?
 
  • #11
JesseM said:
There's a good discussion of how certain effects of gravity "compensate" for the propagation delay here:

http://math.ucr.edu/home/baez/physics/Relativity/GR/grav_speed.html

Has no one noticed how "delay canceling " is a logical paradox?

To say delay gets canceled makes sense as much as if they said distance gets canceled.
blaksheep423 said:
this article sums up what i already knew, but is there any indication that the speed of gravity may not be exactly c? and is it absolutely essential to any standing theory that gravity propagate at the speed of light, or is it conceiveable that it could be slightly less?

What do you mean? Article very directly states speed of gravity is almost instantaneous. That is nowhere even close to the speed of light. Article says:
- "In the simple Newtonian model gravity propagates instantaneously"

- "The net result is that the effect of propagation delay is almost exactly cancelled, and general relativity very nearly reproduces the Newtonian result."v= s/t
v= s/delay

v= s/(delay - delay_almost_exact_cancel)
v= ~s/0.000000000000000000000000000000000000000000000001 Speed of gravity seem to be adjusting itself so it can act "almost instantaneously" regardless of distance. -- Has no one considered that gravity fields could be a fixed-part of the elementary particles and not something that propagates from it. Like a rigid-body fields would then move along with its center and that would explain instantaneous action over distance. How about it?
 
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  • #12
Estif said:
Has no one noticed how "delay canceling " is a logical paradox?

To say delay gets canceled makes sense as much as if they said distance gets canceled.
Not if you pay attention to the context. In this case, they are saying that the delay that would be present in a hypothetical theory of gravity where the force vector always points to an object's "retarded" position (i.e. the position it was at when it was emitting a signal moving at the speed of light which would just be reaching you at this moment) is canceled out when you calculate the actual direction of the gravitational pull in the "weak field" approximation to GR (or at least, it is canceled for objects moving at constant velocity).
 
  • #13
Creator said:
Van Flandern and others do bring up some valid counter points... (PLEASE, folks; no flaming about Van Flandern...that is NOT the point here.)

Then I am afraid you shouldn't have brought him up.

I've actually had lunch with Tom van Flandern. He is a true gentleman. Unfortunately, he's also an object lesson in what happens when one becomes too enamored of one's own theory. During the course of this lunch, when presented with a counter-argument told me that this proves that not only is GR wrong, but Newtonian mechanics is wrong as well.

You simply cannot take Tom van Flandern to be a reliable source.

You will not learn anything whatever about the speed of gravity by looking at orbits around a static gravity source. The source is static. Specifically, the potential is just a function of distance, and the force is just the gradient of the potential. The relevant time scale is not the 8 minutes it takes gravity to reach the Earth from the sun, it's the 4.5 billion years the sun has been here.

All this talk of aberration and remarkable cancellations, while true, is simply an artifact of working in a geocentric frame, where things are a mess. In a heliocentric frame, everything looks simple - there's a static potential, which has a gradient, the force, and the Earth responds to this force.

Measuring the speed of gravitational waves is difficult but straightforward. The radiated power depends on the speed of gravitational radiation, and it's straightforward to measure the energy loss in a binary pulsar system. One gets that the speed of gravity is close to and compatible with the speed of light.

Measuring the speed of static gravity (assuming it even can be different from radiation - this is far from clear) is very difficult. You need two large masses, close enough to each other that one's field doesn't dominate, but far enough apart that there is a measurable delay in propagation time - and you need something to act as a test probe to measure the local spacetime curvature. This is incredibly difficult, as few such systems exist, and placing a test probe where you want it adds even more complications. People have tried this using the sun, Jupiter (already not ideal) and EM radiation as a test probe. This has proved to be even more difficult than expected, as the use of EM radiation as the test probe mixes the speed of light into the problem in a non-trivial way, and the interpretation of the results have been controversial.
 
  • #14
Vanadium 50 said:
... The relevant time scale is not the 8 minutes it takes gravity to reach the Earth from the sun, it's the 4.5 billion years the sun has been here.

Are you saying this delay (8 minutes) does not actually get canceled, and so Earth does not orbit Sun, but the point where Sun was 8 minutes ago? What does it matter what happened in the past, is there some accumulative effect that impacts potentials and delays? I thought orbitals depend ONLY on distance, mass and velocity (initial conditions so to say).

What formula are you using instead of F= k* m1*m2/r^2 ?
 
  • #15
Estif said:
and so Earth does not orbit Sun, but the point where Sun was 8 minutes ago?
There is no frame of reference in which this question makes any sense:
- In the frame of the Sun, the Sun and the point where Sun was 8 minutes ago is the same.
- In the frame of the Earth, the Earth does not orbit anything.
 
  • #16
A.T. said:
There is no frame of reference in which this question makes any sense:
- In the frame of the Sun, the Sun and the point where Sun was 8 minutes ago is the same.
- In the frame of the Earth, the Earth does not orbit anything.
Am I correct in understanding that the "weak field" approximation to general relativity treats gravity as a type of field in flat minkowski spacetime? (see p. 468 of this book). If so, can you pick an "inertial" coordinate system where the Sun has some constant velocity and figure out whether the Earth is being accelerated towards its current position at each moment?
 
  • #17
JesseM said:
If so, can you pick an "inertial" coordinate system where the Sun has some constant velocity and figure out whether the Earth is being accelerated towards its current position at each moment?
Yes, right. Stating "There is no frame of reference in which this question makes any sense" was wrong. I just considered the two mentioned frames.

The fact that the Earth is being accelerated towards the inertially moving Sun's current position doesn't imply that the speed of gravitational field propagation is infinite. The field could have a velocity component.
 
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  • #18
A.T. said:
The fact that the Earth is being accelerated towards the inertially moving Sun's current position doesn't imply that the speed of gravitational field propagation is infinite. The field could have a velocity component.
Right...when people like Van Flandern claim the speed is infinite (or faster than c), are they actually claiming gravitational information is traveling faster than light, so if you shake one planet, observers on other planets would feel the gravitational effect earlier than the light from the shaking-event would reach them? If so, could this be debunked just by showing that in GR, the curvature in some finite region of spacetime can be determined by what's in the past light cone of that region, not by anything outside outside the past light cone?
 
  • #19
JesseM said:
If so, could this be debunked just by showing that in GR, the curvature in some finite region of spacetime can be determined by what's in the past light cone of that region, not by anything outside outside the past light cone?

But van Flandern doesn't (well, didn't) believe in GR. Or SR. So he's not going to be convinced by that argument.

Like I said, he's an object lesson in what happens when one loves one's own theories too much. When faced with a contradiction between his theories (intended to preserve Newtonian mechanics) and Newtonian mechanics, he concluded Newtonian mechanics is wrong.
 
  • #20
A.T. said:
There is no frame of reference in which this question makes any sense:
- In the frame of the Sun, the Sun and the point where Sun was 8 minutes ago is the same.
- In the frame of the Earth, the Earth does not orbit anything.

That would be true if those two masses were the only ones in the universe and the distance between them was constant.

A third mass with an orbit in a different plane should make for a very good vantage point to judge what is going on with the first two. From this planet we would still not know if the system is moving or not as a whole, position of the Sun and where Sun was 8 minutes ago would still be the "same", but we should be able to see all the other relations.

But, even if the first two masses were the only ones, without instantaneous action and orbits being exactly around their present centers they would not be able to keep a constant distance and stable orbits, according to Newtonian mechanics, as I've have heard.


However, having a sky full of distant stars it's like having a grid or millimeter paper (absolute reference frame) that can serve as a guide for plotting mathematical functions and deduce relative motion, if not absolute one.


If we can easily measure 8 minutes delay with the light, why can't we do the same with gravity? Eight minutes is quite a delay, and if you try to simulate solar system with this delay, it will fall apart, according Newtonian mechanics, as I have heard.


What formula are you using instead of F= k* m1*m2/r^2?

How do you know it's more correct?
 
  • #21
Vanadium 50 said:
But van Flandern doesn't (well, didn't) believe in GR. Or SR. So he's not going to be convinced by that argument.
Oh, somehow I thought he was saying physicists are misunderstanding what GR says about the speed of gravity on a theoretical level. So what's his deal, he agrees GR predicts gravity travels no faster than light, but thinks there is empirical evidence that it actually does? But for any observation he might point to about how planets move in our solar system, isn't it possible to show that the movements match the predictions of GR, using a weak-field approximation or a numerical approximation or something?
 
  • #22
Vanadium 50 said:
But van Flandern doesn't (well, didn't) believe in GR. Or SR. So he's not going to be convinced by that argument.

Like I said, he's an object lesson in what happens when one loves one's own theories too much. When faced with a contradiction between his theories (intended to preserve Newtonian mechanics) and Newtonian mechanics, he concluded Newtonian mechanics is wrong.

Are scientists equally divided in their opinions about this, or is there a majority? If there is a majority, then what is their explanation, what is their _official document explaining all this?Is there an "official" kind of document for anything in science at all? I mean, we can't even agree if we are to consider a virus living or non-living thing, and I'm pretty sure there are many even more extreme examples of the division of opinions. So, what do we do without majority?

And what do we do if majority is wrong, like in Galileo time?
 
  • #23
Estif said:
But, even if the first two masses were the only ones, without instantaneous action and orbits being exactly around their present centers they would not be able to keep a constant distance and stable orbits, according to Newtonian mechanics, as I've have heard.
Instantaneous action is merely the simplest way to make orbits work like they do, so Newton went with it. This doesn't mean it is the only way or the correct way.

Even without GR, you could modify Newtons gravity field to be non-instantaneous but have a velocity component inherited from the velocity of the field's source. The field lines in such a field emitted from a inertially moving source would point towards the current position of the source, not the position of their emission. See the electric field. No information is transported instantaneously, because the information about the source's velocity was already available at emission time.

I'm not saying that this is a good law of gravity. I'm just pointing out the flaw in the simplistic argument which goes like: "If objects are pulled to the current position of a moving mass, information must travel instantaneously"
 
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  • #24
A.T. said:
Instantaneous action is merely the simplest way to make orbits work like they do, so Newton went with it. This doesn't mean it is the only way or the correct way.

I must agree, somewhat reluctantly though, because as a logical principle Occam's razor would demand that scientists accept the simplest possible theoretical explanation for existing data. It is the same principle that led to abandonment of the aether theories. But yeah, I'm with you... even if all seemed to fit perfectly well, it doesn't hurt to look for an alternative answers or interpretations.
Even without GR, you could modify Newtons gravity field to be non-instantaneous but have a velocity component inherited from the velocity of the field's source. The field lines in such a field emitted from a inertially moving source would point towards the current position of the source, not the position of their emission. See the electric field. No information is transported instantaneously, because the information about the source's velocity was already available at emission time.

You lost me. I like mathematics definitions and formulas most of all, they are much harder to misinterpret than worded theories, so if you can point some link where this is explained in a bit more depth?
I'm not saying that this is a good law of gravity. I'm just pointing out the flaw in the simplistic argument which goes like: "If objects are pulled to the current position of a moving mass, information must travel instantaneously"

I agree, but I do not see any other explanation. So, what can we do?

First we have to assume quite a bit of determinism in this universe. Then, we can measure the real-world and come up with some theories, and these theories we should be able to re-phrase in mathematical formulas.

With this math all we need to do now is to predict the real-world measurements.

Prediction in deterministic universe should be straight forward... if we only had a power of precision, infinite divisibility, parallelism and continuity universe has. In other words, we need to do kinematic simulation, we need to integrate our equation over time and calculate trajectories, but we are bound to have errors.

So, we plug "F=k* m1*m2/r^2" in our numerical integration and we plot trajectories, step-by-step, the smaller the better, and we find this simple equation works remarkably well, especially considering all the imprecision that came in, not only due to limited computer precision, but also due to measurements of initial condition.

Hence, considering all that, this equation makes me happy.

To convince me otherwise, just give me a better equation, that's all.
 
  • #25
Estif said:
I must agree, somewhat reluctantly though, because as a logical principle Occam's razor would demand that scientists accept the simplest possible theoretical explanation for existing data.
Yes, but instantaneous Newtonian gravity doesn't explain all existing data: amount of light bending, orbit precession.

Estif said:
You lost me. I like mathematics definitions and formulas most of all, they are much harder to misinterpret than worded theories, so if you can point some link where this is explained in a bit more depth?
Take the electric field of an inertially moving electron. Even at a distance the field lines always point to the current position of the electron. Yet if the electron suddenly stops you see that the information about the stop propagates only at c. At distant points the field lines still point to the extrapolated position where the electron would be, if it didn't stop.
On the electric field;
http://farside.ph.utexas.edu/teaching/em/lectures/node125.html
Similar discussion on gravity:
https://www.physicsforums.com/showthread.php?p=2270590
 
  • #26
"If objects are pulled to the current position of a moving mass, information must travel instantaneously"

Imagine gravity fields as a fixed extension of elementary particles and not something that propagates from it. Like a rigid-body fields would then move along with its center (like a soccer ball), all at once, though during the interaction there would still might be some delay depending on the rigidity, flexibility or compressibility of this field, but the propagation of this force does not need to be similar to EM waves at all.

EM waves I imagine as ripples in this gravity field "material", but this medium built from gravity fields could still have its non-compressibility, like water, so it could propagate waves at one speed, but transmit a displacement or friction action at different speeds.Does this make sense? Is there any theory based on similar idea?[EDIT]
Hey, there you are... I see links, thanks a lot. Catch you latter.
 
  • #27
Estif said:
Are scientists equally divided in their opinions about this, or is there a majority? If there is a majority, then what is their explanation, what is their _official document explaining all this?

There is no "Official Document of Science", and if there were, it would certainly not be devoted to refuting bad arguments. Van Flandern's argument is simply incorrect - it doesn't measure what he says it measures.

Even if one doesn't know the "right" answer doesn't mean that one can't spot a bad argument.

Estif said:
And what do we do if majority is wrong, like in Galileo time?

And speaking of bad arguments, this one is a doozy. Jim Lippard, I think summed it up best: "Yes, they laughed at the Wright Brothers. But they also laughed at Laurel and Hardy."
 
  • #28
Vanadium 50 said:
And speaking of bad arguments, this one is a doozy. Jim Lippard, I think summed it up best: "Yes, they laughed at the Wright Brothers. But they also laughed at Laurel and Hardy."

And Laurel and Hardy were right! :smile:
 
  • #29
I have no problem in my mind with Earth being attracted to the point where the Sun was 8 min ago. Of course frame dependent "floating" of common centre of mass arises, but it is not hard to imagine how it cancels out if you make a special case of velocity vector laying in a orbital plane.

But I have whole other issue with gravity propagation being equal to C, and that is how on the largest scales gravity is not doomed to fade away completely towards the edge of OU, just as light is. After all gravitational waves are redshifted through expansion just as light waves are, or not?
 
  • #30
A.T. said:
Yes, but instantaneous Newtonian gravity doesn't explain all existing data: amount of light bending, orbit precession.

When did they come up with the conclusion about precession, what year?

Who simulated it? What was the size of the time-step and what kind of integration algorithm were they using? Did they take the size of the planets into account? Did they integrated all the planets and all the moons in this simulation?

If they did everything right maybe they would get the correct precession result.

Bending of light might be EM interaction, rather than gravity related, but otherwise I agree with you, I can not support what I just said, though I would like to see a new attempt at simulating orbit precession with today's computers and data.The problem is that GR produces very similar results as Newtonian gravity with much more dubious interpretation visa vi 'instantaneous action', and I don't even know what is that interpretation if it's not the one where delay gets canceled. What are the other interpretations for this "instant" action beside "delay-cancel" one?

I do not even know what formula in GR is supposed to calculate the same thing? What are the inputs, what are the outputs? Do you integrate it over time, or can you get some sort of statistical prediction from only one calculation? How do you input position, velocity and mass in GR equation? How do you setup initial conditions of all the planets and all the moons with GR? How it all works? Can it be simulated on the computer just like with classical physics? What model NASA uses for their trajectories, Newtonian or GR?
Take the electric field of an inertially moving electron. Even at a distance the field lines always point to the current position of the electron. Yet if the electron suddenly stops you see that the information about the stop propagates only at c. At distant points the field lines still point to the extrapolated position where the electron would be, if it didn't stop.
On the electric field;
http://farside.ph.utexas.edu/teaching/em/lectures/node125.html
Similar discussion on gravity:
https://www.physicsforums.com/showthread.php?p=2270590

Why "r^3"? Where did "r^2" go?
How many dimensions are they modeling?In any case, I have to disagree with all that.

I could just as same said this: F(electric)= k* q1*q2/r^2 ...and conclude action is instantaneous, which takes us back to the almost exactly the same formula as with gravity, and so the argument about the delay continues.There is one thing that strikes me as very strange there. They calculate electric force, but they do not calculate magnetic force. Instead, they calculate magnetic _field, but to calculate magnetic _force you need one more cross product with the velocity, and then you get a right-hand rule and what is known as Lorentz force. But even more odd is that they do not use their magnetic field for anything. It's not part of any equation necessary for this conclusion, so it looks strangely superfluous.
 

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