Gravity: How Fast Does it Travel?

[farmer]

Does the force of gravity travel the speed of light? faster than the speed of light? or is it instantaneous?

Is there a distinction between propagating gravity waves and the force itself?

If gravity travels the speed of light, it could not escape a black hole, because the escape velocity is faster than light. So gravity must be faster.

If gravity is faster than light, but finite, wouldn't there exist an event horizon through which gravity could not escape? Depending on the speed of gravity and the density to which matter can compress, could there exist a "gravity hole" that would be undetectable (because no light or gravity can escape) unless it happens to directly collide with something. And would "red-shifted" gravity waves exist as well, due to a high gravity environment or the expansion of space?

One more musing: Do the other forces of nature have speeds, such as the electric, strong, and weak forces?

 

[G01]

The Gravitational force as well as the electromagnetic force both travel at the speed of light. (I cannot comment on the other two forces with certainty, but I believe this is true for them as well.)

Your question about gravity escaping a black hole does not make much sense to me. Gravity is what keeps things inside a black hole. It seems to me that you are treating gravity as something else which is affected by gravity! Gravity does not pull on itself, so this question does not make much sense to me, maybe someone more versed in these topics can help you out if I'm missing something.

 

[Robert J. Grave]

The proper way to think of gravity is a change or distortion of the shape of space/time in the presents of mass/energy. This view was first expressed by Einstine in his general therory of relativity. This shape is what causes a satelite to move around a planet in an eliptical path instead of a straight line. the satelite is actually following the path of least resistance and a force would be required to keep it from the curved path. The shape of space/time around the body is always there with it and its' influance extends indefinately but is reduced by the square of the distance from the body. Gravity is not a force and is the same thing as inertia, two aspects of the same thing. When you change direction in a car you feel a force which is actually Your body trying to NOT change direction. The so called force of gravity is the same thing, the change from the natural curved path. In orbit, you feel no force, unless you fire a rocket and change your path. -Robert

 

[MeJennifer]

Assuming you talk about the theory of general relativity then:

Does the force of gravity travel the speed of light? faster than the speed of light? or is it instantaneous?

Gravitational waves travel at the speed of light.

Is there a distinction between propagating gravity waves and the force itself?

No.

If gravity travels the speed of light, it could not escape a black hole, because the escape velocity is faster than light. So gravity must be faster.

A black hole is a gravitational field. There is nothing to escape.

 

[farmer]

Thank you for the replies. I'm thinking about it wrong. Gravity does not interfere with itself (except perhaps when gravity waves cross paths just as when light waves cross paths). I was just thinking since photons are affected by gravity, maybe gravity waves and gravitons would be too.

Also, it is a good observation that gravity is a curvature in space-time.

I will continue to ponder gravity.

 

[MeJennifer]

Gravity does not interfere with itself (except perhaps when gravity waves cross paths just as when light waves cross paths).

Gravitational fields do interfere with each other.

Take two gravitational fields, as soon as their light cones cross they will interfere with each other and create a resulting gravitational field.

 

[keinve]

gravity's influence is technically finite, though not if you count black holes. a singularity is infinintly dense, so it's gravitational influence is infinite. it's just the range that the gravity works on that is affected. once you take out black holes, gravity is finite. it depends on how dense the object is. if the Earth were compressed to the size of roughly a golf ball, the gravitational effects would be similar to a black hole, in that it would not allow light to escape. so to answer your question, the effects of gravity are in direct proportion to to density, and how far it goes is in direct proportion to overall size.

 

[bassplayer142]

I think what he is trying to get at is that the force of gravity extends through the black hole. As in, he is trying to figure out at what distance an object could be away from the black hole to where the black hole exerts no force on the object. If so then the answer is infinity because everything in the universe is exerting gravity on everything else, even at a great great distance, gravity exerts on other masses on a microscopic level.

It is kind of interesting too because gravity can travel through anything. Through any mass and medium all the way across the galaxy at every natural extreme.

 

[pervect]

Why the necropost (post to an old dead thread)?

Anyway, I'd suggest starting by reading the FAQ:

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

 

[pallidin]

Gravitational influence has never been shown to exceed or go below C. However, this is not set in stone... the complexities involved demand invesigating in this mystery.

 

[George Jones]

Gravitational influence has never been shown to exceed or go below C. However, this is not set in stone... the complexities involved demand invesigating in this mystery.

I posted a little elaboration on this here.

 

[jostpuur]

The Gravitational force as well as the electromagnetic force both travel at the speed of light. (I cannot comment on the other two forces with certainty, but I believe this is true for them as well.)

Somebody could confirm this in one direction or another. I've thought that the fields of the nuclear interactions propagate below the speed of light.

hmhm... I wasn't thinking this carefully. The disturbances in KG fields propagate everywhere in the light cone, but on the other hand wave packets will travel with speeds below c if m!=0. I guess the question isn't simple enough to be given a simple answer.

In fact I don't know what kind of fields are used for nuclear forces, but are they something similar to the Klein-Gordon fields?

 

[QuantumPion]

I think what he is trying to get at is that the force of gravity extends through the black hole. As in, he is trying to figure out at what distance an object could be away from the black hole to where the black hole exerts no force on the object. If so then the answer is infinity because everything in the universe is exerting gravity on everything else, even at a great great distance, gravity exerts on other masses on a microscopic level.

It is kind of interesting too because gravity can travel through anything. Through any mass and medium all the way across the galaxy at every natural extreme.

What if gravity is quantized (gravitons)? In this case wouldn't there be a minimum unit for gravitational force, e.g. one graviton? So if you were far enough away from a mass, you would receive no gravitons and thus no force. Or looking at it another way, if a gravity well was actually a staircase, there would be a "top" of the stair case with maximum potential.

 

[pervect]

What if gravity is quantized (gravitons)? In this case wouldn't there be a minimum unit for gravitational force, e.g. one graviton? So if you were far enough away from a mass, you would receive no gravitons and thus no force. Or looking at it another way, if a gravity well was actually a staircase, there would be a "top" of the stair case with maximum potential.

Electromagnetism is quantized. Yet there is no "top of the staircase" effect such as you describe in E&M.

One thing you have to realize is that just as the coulomb force between two charges is carried by virtual photons, the "gravitational force" would (probably) be carried by virtual gravitons. Note that even this may be an oversimplification.

AFAIK there isn't any "minimum value" for the energy or momentum of a virtual photon

So my general advice is to first get your ducks in a row for E&M, and then move on to gravity later.

You might try http://www.math.ucr.edu/home/baez/physics/Quantum/virtual_particles.html

for some info on how virtual particles carry forces

Gravity related links are
http://www.math.ucr.edu/home/baez/physics/Relativity/GR/grav_speed.html

on the speed of gravity

http://www.math.ucr.edu/home/baez/physics/Relativity/BlackHoles/black_gravity.html
on "gravity getting out of a black hole".

Note that since GR is a classical theory, it doesn't have to deal with these issues. As the FAQ says:

Purely in terms of general relativity, there is no problem here. The gravity doesn't have to get out of the black hole. General relativity is a local theory, which means that the field at a certain point in spacetime is determined entirely by things going on at places that can communicate with it at speeds less than or equal to c. If a star collapses into a black hole, the gravitational field outside the black hole may be calculated entirely from the properties of the star and its external gravitational field before it becomes a black hole. Just as the light registering late stages in my fall takes longer and longer to get out to you at a large distance, the gravitational consequences of events late in the star's collapse take longer and longer to ripple out to the world at large. In this sense the black hole is a kind of "frozen star": the gravitational field is a fossil field. The same is true of the electromagnetic field that a black hole may possess.

Often this question is phrased in terms of gravitons, the hypothetical quanta of spacetime distortion. If things like gravity correspond to the exchange of "particles" like gravitons, how can they get out of the event horizon to do their job?

Gravitons don't exist in general relativity, because GR is not a quantum theory. They might be part of a theory of quantum gravity when it is completely developed, but even then it might not be best to describe gravitational attraction as produced by virtual gravitons. See the physics FAQ on virtual particles for a discussion of this.

 

[rbj]

i realize that this appears to be a resurrected post (or maybe it's a zombie post, if the sysops shoot it, will it die?), but i would be curious to see some response to this:

Do the other forces of nature have speeds, such as the electric, strong, and weak forces?

of course the "electric" force (EM) has, by definition, a speed of c.

but my understanding from SR and GR is that it is not just gravity (or the perturbation of space-time) and EM that move at a speed of c, but all interaction, otherwise information could move at the speed of the other fundamental interaction. is that not correct?

From discussions with some pretty heavy physicists (it's sort of amazing whom you can talk to, if you find their email address), the understanding from them that i gleaned was this: Nature has a single finite speed for these interactions (which may someday be all unified in a single theory). The salient physics is that speed is the same for all fundamental interactions and that it is finite. That is, whatever the interaction, if something changes over here, the effect over there, as observed by a third party somewhere else (but let's say equidistant from here and there), will happen at a time that is delayed by

\frac{ \left| \mathrm{locus}(here) - \mathrm{locus}(there) \right| }{c}

where c is that finite speed.

now the salient fundamental physics is that this speed of propagation, c, is finite, not infinite. physical reality would be different than it is if c were infinite. but it doesn't really matter what that finite speed is since it, along with G and \hbar, will simply define the scale of existence of things in the universe. as long as all of the dimensionless parameters of interaction remain the same (physicist John Baez has enumerated 26 such dimensionless parameters, but says there could be more as new interactions are discovered and that new physical theories might derive some of these parameters from others, thus reducing that number), a conceptual change in c could not be noticed by observers whose existence and scale is governed by that.

my interpretation: if God (or some "god-like" being) could reach over and turn the knob that controls c to half of its previous value so the new c is the old c/2, then the Planck Length would increase by a factor of \sqrt{8} and so would the size of atoms, meter sticks, and people (from the POV of this "god-like" observer) if all the dimensionless parameters remained the same. but, also, the Planck Time would increase by a factor of \sqrt{32} (from the perspective of this "god-like" observer) and, if all the dimensionless parameters remained the same, all of our clocks would have to tick slower by the same factor. so this "god-like" observer might observe that the speed of propagation of EM (and the other interactions) now is half of what it used to be, but for us that exist within the governing of physics, we could not tell any difference. light would still travel 299792458 of our new meters in the time elapsed by our new second. nothing operationally would change. from the POV of our existence, no new physics would be observed.

so if you're a theist (and running with this hyperbolic or parabolic imagery), God doesn't have a control knob on His/Her toy (that we call "The Universe") labeled "c", but He/She/It/whatever, might have one labeled "\alpha" and, perhaps 25 other such knobs (say for the cosmological constant or the masses of particles, all expressed in something like Planck units). i dunno, of course, it's just a speculative imagery that i found useful to think about what universal constants really matter and which ones do not (that is they only reflect our choice of units).

 

[pervect]

i realize that this appears to be a resurrected post (or maybe it's a zombie post, if the sysops shoot it, will it die?), but i would be curious to see some response to this:



of course the "electic" force (EM) has, by definition, a speed of c.

but my understanding from SR and GR is that it is not just gravity (or the perturbation of space-time) and EM that move at a speed of c, but all interaction, otherwise information could move at the speed of the other fundamental interaction. is that not correct?

Right.

from discussions with some pretty heavy physicists (it's sort of amazing whom you can talk to, if you find their email address), the understanding from them that i gleaned was this: Nature has a single finite speed for these interactions (which may someday be all unified in a single theory). The salient physics is that speed is the same for all fundamental interactions and that is finite. That is, whatever the interaction, if something changes over here, the effect over there, as observed by a third party somewhere else (but let's say equidistant from here and there), will happen at a time that is delayed by

|locus(here) - locus(there)|/c

where c is that finite speed.

now the salient fundamental physics is that this speed of propagation, c, is finite, not infinite. physical reality would be different than it is if c were infinite. but it doesn't really matter what that finite speed is since it, along with G and \hbar, will simply define the scale of existence of things in the universe. as long as all of the dimensionless parameters of interaction remain the same (physicist John Baez has enumerated 26 such dimensionless parameters, but says there could be more as new interactions are discovered and that new physical theories might derive some of these parameters from others, thus reducing that number), a conceptual change in c could not be noticed by observers whose existence and scale is governed by that.

my interpretation: if God (or some "god-like" being) could reach over and turn the knob that controls c to half of its previous value so the new c is the old c/2, then the Planck Length would increase by a factor of \sqrt{8} and so would the size of atoms, meter sticks, and people (from the POV of this "god-like" observer) if all the dimensionless parameters remained the same.

I'm not sure if I understand this. I was under the impression that if all the dimensionless parameters remained the same, the value of 'c' didn't matter, there was no new physics. I.e you could change 'c' to 'c/2' by doubling the length of the meter and leaving the second the same. This would double the size of atoms (I'm not sure where you got sqrt(8) - I would assume you had some sort of rationale, but that's not what I would guess would happen) You could also change 'c' to 'c/2' by doubling the length of the second - in this case, atoms would remain the same size, but the units of time would vary.

 

[rbj]

Right.

that's reassurring. i am trying to not misquote or mis-contextualize any of these pearls that i get from emails with the likes of Michael Duff or Lev Okun or Gabriel Veneziano. and if i f*ck something up, i want to know.

I'm not sure if I understand this. I was under the impression that if all the dimensionless parameters remained the same, the value of 'c' didn't matter, there was no new physics.

that's what i understand, too.

I.e you could change 'c' to 'c/2' by doubling the length of the meter and leaving the second the same. This would double the size of atoms (I'm not sure where you got sqrt(8) - I would assume you had some sort of rationale, but that's not what I would guess would happen)

I was assuming an unchanged G and \hbar (as well as the dimensionless parameters, which are the important ones). if c was halved, the Planck Length would increase by \sqrt{8} (from the POV of the outside observer that is ungoverned by physics and who, hypothetically, could actually observe c getting cut in half) and if all the dimensionless ratios remained constant, so would atoms, meter sticks, and every other length. the Planck Time (from the POV of the outside observer that is ungoverned by physics) would be increased by a factor of \sqrt{32}. light would travel half as fast (from the POV of this supernatural observer), and would need to travel \sqrt{8} times farther, but would have a factor of \sqrt{32} = 2 \sqrt{8} more time to do it. assuming the dimensionless ratios of meter/PlanckLength and second/PlanckTime remain the same, this comes out to be the same number of new meters per new second.

so, in this thought experiment, if you, as this "god-like" observer/manipulator would "change 'c' to 'c/2' by doubling the length of the meter [and atoms] and leaving the second the same", but then (assuming the number of atoms in the meter stick remain constant) the dimensionless ratio of the atom sizes (approximately the Bohr radius) to the Planck Length would change (which is outside the axiom) if the dimensionless ratio of the second to the Planck Time remained the same. so i don't think that quite works, Pervect. if the second (and Planck Time) remained the same while c was cut in half the G \hbar product would have to decrease by a factor of 32 but if the meter (and Planck Length) was doubled while c was cut in half, then the G \hbar product would decrease by a factor of 2. 32 is not equal to 2. and I'm assuming that the number of atoms in the meter stick does not change, the number of Planck Lengths in the size of the atoms do not change, and the number of Planck Times per "period of the radiation corresponding to the transition between the two hyperfine levels of the ground state of the caesium-133 atom" remains the same.

You could also change 'c' to 'c/2' by doubling the length of the second - in this case, atoms would remain the same size, but the units of time would vary.

how can either doubling the length of the meter or doubling the length of the second both have the same effect to change c to c/2?Edit: i thought about this a little, and i think what you meant to say, Pervect, is that you can change c to c/2 by halving the length of the meter (and the Planck Length), leaving the second (and Planck Time) unchanged, or you can change c to c/2 by leaving the meter unchanged and doubling the length of the second. That works, but besides a changing value of c (from the POV of the unaffected supernatural observer), there would also be changing G and/or \hbar. in any case, light, E&M, gravity, whatever interaction, will continue to travel 1 Planck Length during the period elapsed by 1 Planck Time.

 

[pervect]

OK, I see where you're coming from now: if you assume that G and hbar remain constant, the Planck length is just

\sqrt{\frac{G \bar{h}}{c^3}}

so that's where your factor of sqrt(8) came from.

As far as what I had in mind, if 1 new meter = 2 old meters, then

c = 3e8 old meter / second = 1.5e8 new meter / second

so doubling the meter halves the "speed of light" from 3e8 "old meters" per second to 1.5e8 "new meters"/ second.

 

[rbj]

OK, I see where you're coming from now: if you assume that G and hbar remain constant, the Planck length is just

\sqrt{\frac{G \bar{h}}{c^3}}

so that's where your factor of sqrt(8) came from.

As far as what I had in mind, if 1 new meter = 2 old meters, then

c = 3e8 old meter / second = 1.5e8 new meter / second

so doubling the meter halves the "speed of light" from 3e8 "old meters" per second to 1.5e8 "new meters"/ second.

that doesn't quite work for me. i think that, if all of the dimensionless parameters remain constant,

c = 299792458 old_meters/old_second = 299792458 new_meters/new_second

and the new_second cannot be the same as the old_second if the meter had changed.

but i think we (as well as Duff) agree: ain't no operational difference. a change in c (or in G or h or any other sole dimensionful "constant") is not merely impossible, but is functionally meaningless.

i still don't know what to think of this inflationary universe theory where the universe expands faster than c at some time in its past.

 

[yogi]

Several of the comments re the speed of fields are not established by experiment - the speed of light in a vacuum is c, we all know that, but the speed with which a closed non-divergent magnetic field propagates in a loop of magnetic material is not readily explainable in terms of the field starting out at each pole of the energized magnet and meeting itself somewhere in middle - waves go from place to place - we do not know the mechanism by which fields make their forces felt at a distance -

It seems when physics needs to explain quantum entanglements and virtual photons the speed barrier is shunted to the side. In the case of gravity, it is usually assumed there is a graviton exchange between attracted particles - but gravity and inertia may be the result of global dynamics - the cosmological constant or, like expansion, an ongoing change that does not happen at one place and travel to another, but rather something that affects spacetime continuously. The curvature of GR may be the result of local mass interaction therewith, in which case it may not be meaningful to assign a propagation velocity to the curvature.

 

[pervect]

Several of the comments re the speed of fields are not established by experiment

The speeds are certainly established by theory, though. And the theory has survived every experimental test thrown at it, to date.

For instance, if Maxwell's equations were wrong, we'd start to see disagreement with experiment, even if that experiment wasn't directly designed to measure some sort of "speed".

Maxwell's equations certainly give us a good reason to expect that electromagnetism, in general, travels at 'c' in the general sense that if you change something "here", it won't have any effect "there" until after a delay of at least c/distance.

Some care does need to be taken as to what means by speed. Specifically, one has to use the above defintion, and not try and guess the speed from the direction of the coulomb force, a common sorce of confusion that is also often repeated in "speed of gravity" threads.

GR is no different as far as the theoretical aspects go. (However, we don't have any direct measurements of the speed or even the existence of gravity waves, while of course we do have direct observations of light).

The equations are a lot messier than Maxwell's equation, but there is proof that GR is a well posed initial value problem, which implies that the "fields" propagate at less than 'c'. (You can regard the "fields" as changes in the metric, which will also change the Christoffel symbols and the curvature tensor).

The details of the proof that GR is a well posed initial value problem are rather complicated and I'm not especially familiar with them, but you can find the proof in Wald, "General Relativity". I've written a little about this in the past, as to what it means to be a well-posed initial value problem and what this implies about propagation speed.

 

[yogi]

The speeds are certainly established by theory, though. And the theory has survived every experimental test thrown at it, to date.

For instance, if Maxwell's equations were wrong, we'd start to see disagreement with experiment, even if that experiment wasn't directly designed to measure some sort of "speed".

Maxwell's equations certainly give us a good reason to expect that electromagnetism, in general, travels at 'c' in the general sense that if you change something "here", it won't have any effect "there" until after a delay of at least c/distance.

Would concur - there is much indirect/consequential evidence of c as the limiting communication velocity - but being the eternal skeptic, I always find myself compelled to comment when absolute assertions are made about propagation rates of fields

I sort of expected Eugene to jump into this thread somewhere as he has written a couple of papers on the subject

 

[DaveC426913]

gravity's influence is technically finite ... once you take out black holes, gravity is finite.

Do you mean in terms of distance? No it's not. It's infinite.

 

[rbj]

gravity's influence is technically finite, though not if you count black holes. a singularity is infinintly dense, so it's gravitational influence is infinite. it's just the range that the gravity works on that is affected. once you take out black holes, gravity is finite.

Do you mean in terms of distance? No it's not. It's infinite.

i thought he meant in terms of magnitude of field (or the degree of curvature of space-time).

 

[haushofer]

I haven't read the whole topic, but wat I was wondering, is if there are people who did some calculations about the speed of gravitational waves without the linearization, so for arbitrary large gravitational fields. The calculations for linear fields I understand, but how would one be sure if this speed is the same for arbitrary fields? Why is it still possible to write down a wave equation for the metric field ?

 

[pervect]

I haven't read the whole topic, but wat I was wondering, is if there are people who did some calculations about the speed of gravitational waves without the linearization, so for arbitrary large gravitational fields. The calculations for linear fields I understand, but how would one be sure if this speed is the same for arbitrary fields? Why is it still possible to write down a wave equation for the metric field ?

Yes, Wald talks about this in the context of whether or not gravity is "a well posed initial value problem".

 

[Phred101.2]

Gravity is one if the unexplained "forces", and we know it has a symmetry with EM and "charge". We also know that matter -waves, give off waves -photons from bound electrons (and electrons can do this if they move fast enough); and we know about this other extremely unstable property (superposition) that, unlike the others, seems to ignore space (it's null-spatial).

Is there possibly some symmetry between gravity (an extremely stable, spatial "force" of matter), and superposition -an extremely unstable, non-spatial "force" of some kind??

 

[haushofer]

Yes, Wald talks about this in the context of whether or not gravity is "a well posed initial value problem".

Ok, I can remember such discussions, Carroll also pays attention to it. I will take a look at those texts. If i remember it correctly it was about cutting the space time into slices, and that one tries to describe the evolution at every hypersurface. But how can one proof that one is always able to write down wave equations for the metric, from the field equations? If this question is answered in Wald, I will find out soon :)

 

[pervect]

Yep, that's the sort of thing. Part of what comprises "well posedness" includes the "domain of dependency" on initial values.

 

[Phred101.2]

some symmetry between gravity (an extremely stable, spatial "force" of matter), and superposition -an extremely unstable, non-spatial "force"

There's a symmetry in our understanding (or lack thereof), of the two...?
But it's "broken" if gravity "acts" at the speed of light which is distance-dependent, and superposition, which is independent of distance, acts instantaneously? A true symmetry would mean both were instantaneous "forces" (independent of spatiality) -as Sir Isaac believed...

 

[Salman2]

Reading this old thread..but..what is the correct answer to the OP question ?:

OP Question: How fast is gravity?

==

Does gravity have a "speed" ? Is it fast or slow ?

It does not seem correct to me that we can say "gravity" is fast or slow. Seems to me it would be the object of motion (particle and/or wave) that is fast or slow. Thus, a fast particle/wave is one that moves much in a short period of time, slow particle/wave moves little in a long period of time. Some particles/wave (such as photons) always move the same distance in any period of time and are thus neither fast or slow, they move at c = speed of light. What am I missing in my understanding ?

 

[bcrowell]

Salman2, this thread has been dead since 2007. The speed being referred to by the OP was the speed at which gravitational waves propagate, not the speed of material particles.

 

[Salman2]

Salman2, this thread has been dead since 2007. The speed being referred to by the OP was the speed at which gravitational waves propagate, not the speed of material particles.

OK thanks.

What was the conclusion of the discussion--what is the speed at which gravitational waves propagate--is it c, the same speed that photon wave propagates ?

 

[bcrowell]

What was the conclusion of the discussion--what is the speed at which gravitational waves propagate--is it c, the same speed that photon wave propagates ?

I haven't read the whole discussion, but that is the correct answer.

 

[Star Drive]

Here is a thought experiment about a way to perhaps detect gravity waves.

All around the Earth at strategic points, attach transducers to solid bedrock. These transducers would output electrical waves in response to mechanical waves in the Earths crust, much like a seismometer. However, the sensitivity would be greater and the response would be faster. All transducers would be data linked and digitally time phase adjusted back to a common data processing center for simultaneous processing.

With very close time coordination, remote detonate about a 100 Megaton H-Bomb directly against the Moons surface.

Could we expect to pick up a "ping" and possibly "ringing" in the Earths crust from gravity wave coupling all the way from the moon?

I don't have a clue for how to analyze this.

I'm not a physicist, so go easy on me.

 

[Ich]

Could we expect to pick up a "ping" and possibly "ringing" in the Earths crust from gravity wave coupling all the way from the moon?

Not a chance. Gravity waves, even of some decent astrophysical events (not a feeble H-Bomb) are very very very weak. You need a very high quality resonator with the correct resonance frequency to see, well, still nothing, but no by these orders of magnitude.

 

[Star Drive]

Not a chance. Gravity waves, even of some decent astrophysical events (not a feeble H-Bomb) are very very very weak.


Good point.

However if two neutron stars in mutual orbit, merge on the far edge of the Milky Way, their gravity 'disturbance' would diminish by inverse square law over about a 100K light years.

Would the effect as received on Earth from the merger be more or less than that of an H-Bomb on the moon, which is tightly coupled to the Earth (relatively)?

Its all relative and I know its all in the numbers.

Thanks for your feedback.

 

[B1ffB0ff]

I know its old, but then so is time... :-)

If Gravity, the affacts of a body in space time, are infinite (exerted on all points in the universe at the same time to a greater or lesser extent dendent upon distance from the body) , then the speed at which the affcets can be experinced cannot be limited to C! So hypertheticaly, we remove the moon instanateoulsy, will the tides stop instantly or after a minute or so in reation to C?

Cheers

JB

 

[DaveC426913]

I know its old, but then so is time... :-)

If gravity's effect on a body in space time are infinite (exerted on all points in the universe at the same time to a greater or lesser extent dependent upon distance from the body)

Your supposition is false. While it does have an infinite extent, changes to the gravitational field are limited to propagating at c.

, then the speed at which the effects can be experienced cannot be limited to c! So hypothetically, we remove the moon instantaneously, will the tides stop instantly or after a minute or so in relation to c?

Cheers

JB

You cannot remove a mass instantaneously. It doesn't work that way. The mass would be limited to movement below the speed of light.

However, even if it were not so, the change in gravitational force felt by the disappearance of the Moon would take time to propagate. It takes about 1.2 seconds.

Same with the sun. If the sun suddenly fell through a wormhole and disappeared, we would neither see it nor feel for 8 minutes.

 

[B1ffB0ff]

So, that being the case we should be able to prove this then...

A variation of the other much older experiment with two large mass objects suspended next to each other and the attraction force between them. However.

Main difference we have a massive object suspended (100m) above a smaller weight placed on a very sensitive set of scales, capable of sampling in microseconds.

Allow the high mass object to fall on the much less mass object and the scales.

Film it with a high frame rate camera and time with v accurate clock.

Will need to be located in geologically stable area, maybe in a near vacuum to eliminate affects of air movement.

We should see the measurement of the weight of the small mass object reduce slightly as the high mass object gets closer, further this effect should be measurable against C in proportion to distance, relative to the observer.

Thoughts?

JB

 

[Ryan_m_b]

So, that being the case we should be able to prove this then...

A much easier experiment would be to observe a large, distant mass such as Jupiter with both a telescope and something to measure gravity (gravitational interferometer?). If gravity is instantaneous the latter instrument should tell us it is further along its orbit than the former.

 

[atyy]

A variation of the other much older experiment with two large mass objects suspended next to each other and the attraction force between them. However.

Main difference we have a massive object suspended (100m) above a smaller weight placed on a very sensitive set of scales, capable of sampling in microseconds.

Allow the high mass object to fall on the much less mass object and the scales.

Film it with a high frame rate camera and time with v accurate clock.

Will need to be located in geologically stable area, maybe in a near vacuum to eliminate affects of air movement.

We should see the measurement of the weight of the small mass object reduce slightly as the high mass object gets closer, further this effect should be measurable against C in proportion to distance, relative to the observer.

A much easier experiment would be to observe a large, distant mass such as Jupiter with both a telescope and something to measure gravity (gravitational interferometer?). If gravity is instantaneous the latter instrument should tell us it is further along its orbit than the former.

Possibly relevant is George Jones's post #12 of https://www.physicsforums.com/showthread.php?t=562042. He links to Carlip's paper: "By analyzing the motion of the Moon, Laplace concluded in 1805 that the speed of (Newtonian) gravity must be at least 7×10⁶c." Carlip goes on to show why this is consistent with GR, in which gravitational waves travel at c. Evidence for GR's gravitational waves was obtained by Taylor and Hulse.