Does infinite one-way speed of light violate p conservation?

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Suppose for the sake of argument someone said the outward speed of light is infinite and the return speed is c/2, creating a two-way speed of c.

Wouldn't this violate the conservation of momentum?

p = E/c. That means on the way out, the momentum of light would be zero, but on the way back it would be very much non-zero. Shouldn't the momentum be the same both ways if we're to have conservation of momentum?

Any insight at any level is welcomed. Thanks.
 

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  • #2
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You can save it by redefining momentum. Essentially you do a coordinate transformation like (x,t) -> (x,t+xc). It is just a redefinition of the time coordinate without observable consequences.
 
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  • #3
Dale
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Suppose for the sake of argument someone said the outward speed of light is infinite and the return speed is c/2, creating a two-way speed of c.

Wouldn't this violate the conservation of momentum?

p = E/c.
First, in strange frames like that the usual non-tensor formulas may not hold. You would need to re-derive them.

Second, if you write your laws in terms of tensors then they will hold under all coordinates. So the conservation of four-momentum would still be valid. However, in such coordinates you probably wouldn’t be able to clearly identify one component as the energy and the other components as the momentum.
 
  • #4
Sorcerer
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You can save it by redefining momentum. Essentially you do a coordinate transformation like (x,t) -> (x,t+xc). It is just a redefinition of the time coordinate without observable consequences.
Would that have other theoretical consequences?


First, in strange frames like that the usual non-tensor formulas may not hold. You would need to re-derive them.

Does this mean we'd need a new law in the same way that Einstein redefined momentum by multiplying it by γ(u)?


Second, if you write your laws in terms of tensors then they will hold under all coordinates. So the conservation of four-momentum would still be valid. However, in such coordinates you probably wouldn’t be able to clearly identify one component as the energy and the other components as the momentum.

Is what I'm describing then nothing but a coordinate transformation?

I suppose what I am asking is this: would there be no physical difference in the universe or any other laws if the two-way speed of light had a infinite speed one way and c/2 speed the other way?
 
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PeroK
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Suppose for the sake of argument someone said the outward speed of light is infinite ...

What's the definition of infinite speed?
 
  • #6
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Would that have other theoretical consequences?
It would make all calculations much more complicated.
I suppose what I am asking is this: would there be no physical difference in the universe or any other laws if the two-way speed of light had a infinite speed one way and c/2 speed the other way?
We live in this universe. If you make a weird choice of a coordinate system (the one I posted). As you can see, it has no observable consequences.
 
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Dale
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Does this mean we'd need a new law in the same way that Einstein redefined momentum by multiplying it by γ(u)?
Yes, something similar.

Is what I'm describing then nothing but a coordinate transformation?

I suppose what I am asking is this: would there be no physical difference in the universe or any other laws if the two-way speed of light had a infinite speed one way and c/2 speed the other way?
That is correct. There is no physical consequence to the one way speed of light, it is simply a choice of coordinates. In this case, an exceptionally complicated choice of coordinates, but perfectly valid.
 
  • #8
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What's the definition of infinite speed?
Well,
What's the definition of infinite speed?
Well I guess the speed such that the return trip of light is c/2. One that is only possible for outward going light?

Seems a rather symmetry breaking concept, obviously. As others have informed me, it would require a different definition of momentum and/or nasty change in coordinates, but no detectable differences.


I mean I don’t know how else to define it. I certainly don’t want to define it as a limit, because I suspect that might defeat the purpose of my question.
 
  • #9
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Yes, something similar.

That is correct. There is no physical consequence to the one way speed of light, it is simply a choice of coordinates. In this case, an exceptionally complicated choice of coordinates, but perfectly valid.
Okay so in this instance, not every observer would agree upon WHICH leg of travel was infinite, but everyone would agree on the two-way speed.

That seems like it would require a lot more than just altering momentum. Wouldn’t that require a complete rework of Maxwell’s equations, too? Granted, I’m shooting in the dark, but I’m aware you can combine them into a wave equation with speed c. It seems there would need to be a great deal of reworking of the framework for the laws of physics even if the end result yields the same observations.
 
  • #10
Ibix
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What you are doing, exactly, is drawing:
1. Drawing a Minkowski diagram
2. Deleting the horizontal grid lines
3. Drawing 45° lines
4. Shearing the diagram so that the 45° lines are horizontal.
You can always write coordinate transforms to relate vectors and events drawn on one diagram to the other.

It doesn't strictly require a re-write of Maxwell's equations. It requires you to use the tensor form of those equations, wherein "which coordinate system am I using?" gets abstracted out of the maths. You are, of course, free to unabstract (if that's a word) it again in as many different ways as you like and you will get different forms of the equations. But that's a bit like translating a story into a different language - the letters change but the story doesn't.
 
  • #11
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What you are doing, exactly, is drawing:
1. Drawing a Minkowski diagram
2. Deleting the horizontal grid lines
3. Drawing 45° lines
4. Shearing the diagram so that the 45° lines are horizontal.
You can always write coordinate transforms to relate vectors and events drawn on one diagram to the other.

It doesn't strictly require a re-write of Maxwell's equations. It requires you to use the tensor form of those equations, wherein "which coordinate system am I using?" gets abstracted out of the maths. You are, of course, free to unabstract (if that's a word) it again in as many different ways as you like and you will get different forms of the equations. But that's a bit like translating a story into a different language - the letters change but the story doesn't.
Would this still apply if all inertial reference frames agree that one leg of a light pulse’s travel is infinite and the other is c/2? (although not necessarily agree which leg is which)
 
  • #12
Dale
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Wouldn’t that require a complete rework of Maxwell’s equations, too? Granted, I’m shooting in the dark, but I’m aware you can combine them into a wave equation with speed c. It seems there would need to be a great deal of reworking of the framework for the laws of physics even if the end result yields the same observations.
If you wrote Maxwell’s equations in the usual way, yes it would require a lot of reworking. However, if you use tensors then the same equations hold in any coordinate system.
 
  • #13
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Would this still apply if all inertial reference frames agree that one leg of a light pulse’s travel is infinite and the other is c/2? (although not necessarily agree which leg is which)
As long as your coordinates are smooth and invertible (there are no discontinuities and no point has more than one coordinate description - I think that's all that's needed) you can simply work with the tensor form of physical laws. You can also grind out the form of the laws in your chosen system explicitly if you wish.

Does that answer your question?
 
  • #14
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As long as your coordinates are smooth and invertible (there are no discontinuities and no point has more than one coordinate description - I think that's all that's needed) you can simply work with the tensor form of physical laws. You can also grind out the form of the laws in your chosen system explicitly if you wish.

Does that answer your question?
This and all the other posts definitely paint a clear picture.

So in essence, and correct me if I’m wrong, the answer is no: Momentum conservation is NOT violated. It is still conserved in this hypothetical scenario, which means other than simplicity and some assumptions about symmetry in the universe, choosing an equal one way speed and two way speed is just something we choose.
 
  • #15
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Yes. Ultimately this is why all attempts to measure the one-way speed of light fail - the answer is a matter of choice. All of the maths is needlessly more complicated if you make any other choice than the symmetric one, and Occam's Razor favours the symmetric choice, but you are free to make a different choice if you wish.
 
  • #16
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Yes. Ultimately this is why all attempts to measure the one-way speed of light fail - the answer is a matter of choice. All of the maths is needlessly more complicated if you make any other choice than the symmetric one, and Occam's Razor favours the symmetric choice, but you are free to make a different choice if you wish.
Doesn’t that pose a problem for age of the universe estimates that use distant stars as the minimum earliest time? If that light got here instantaneously, then how can we say it is from an object 13 bullion light years away?

Or in other words, wouldn’t other means of determining the age of the universe refute the notion that light can move with an infinite one way speed?
 
  • #17
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Doesn’t that pose a problem for age of the universe estimates that use distant stars as the minimum earliest time?
No. The age of the universe means something specific. It is the spacetime interval of a worldline of a hypothetical inertial particle which has been around since the beginning of the universe and for which the CMBR is isotropic. This quantity is an invariant quantity which is defined using tensors, so its value is independent of the coordinate system.
 
  • #18
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Doesn’t that pose a problem for age of the universe estimates that use distant stars as the minimum earliest time? If that light got here instantaneously, then how can we say it is from an object 13 bullion light years away?

Or in other words, wouldn’t other means of determining the age of the universe refute the notion that light can move with an infinite one way speed?
You're moving beyond SR here, so some care is needed. We aren't using reference frames any more, and speeds over long distances aren't really well defined. However, your point is generally correct - the age of the universe depends on your choice of coordinates because the definition of "the universe" depends on your choice of coordinates. The age usually quoted is the proper time shown by a clock that always saw the universe as isotropic (CMB is the same colour in all directions). That is the maximum age you can get and is invariant, as Dale says.
 
  • #19
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No. The age of the universe means something specific. It is the spacetime interval of a worldline of a hypothetical inertial particle which has been around since the beginning of the universe and for which the CMBR is isotropic. This quantity is an invariant quantity which is defined using tensors, so its value is independent of the coordinate system.

You're moving beyond SR here, so some care is needed. We aren't using reference frames any more, and speeds over long distances aren't really well defined. However, your point is generally correct - the age of the universe depends on your choice of coordinates because the definition of "the universe" depends on your choice of coordinates. The age usually quoted is the proper time shown by a clock that always saw the universe as isotropic (CMB is the same colour in all directions). That is the maximum age you can get and is invariant, as Dale says.

Darn. I was hoping for a silver bullet lol. I suppose it hasn't been done yet and it probably never will.
 
  • #20
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You have to connect speeds to something concretely measurable. Otherwise, you can achieve your alternative physics by just redefining your coordinates.

Start with coordinates ##x, t##. Define a new time coordinate ##T## via:

##T = t - \frac{x}{c}##

In the new coordinate system, ##x,T##, the speed of light will be ##\infty## in one direction and ##\frac{c}{2}## in the other direction.
 
  • #21
pervect
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Suppose for the sake of argument someone said the outward speed of light is infinite and the return speed is c/2, creating a two-way speed of c.

Wouldn't this violate the conservation of momentum?

I assume you're just trying to think about how physics would work with a clock synchornization convention that's not Einsteinian. But perhaps I'm wrong about that.

Assuming that that is your motivation, though, as a matter of semantics I would say that momentum still exists as a conserved physical quantity, it's just no longer given by the relationship p=mv, but by some other relationship.

For any massive object, for instance, it's possible to define momentum in a relativistically correct manner as mass * proper velocity, where proper velocity is the distance an object moves (measured in a particular frame of reference) divided by the proper time takes for the object to move said distance. Note that this proper time interval does not depend on any frame of reference, as it's independent of the observer.

If the concept of proper velocity is unfamiliar, wiki has a short discussion of it <<link>>.

This won't work for calculating the momentum of light, but it will give the correct answer for momentum for any object moving slower than light, in a manner that's independent of any clock synchronization convention used. You didn't mention clock synchronization explicity, but of course it's the Einstein clock synchronziation convention that makes the speed of light the same in both directions.

It's routine to define the energy-momentum 4-vector as mass * proper velocity. And it's fairly routine to note that the energy momentum 4-vector contains the energy and the momentum 3-vector. So a lot of it is semantics and what one is used to.
 
  • #22
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I assume you're just trying to think about how physics would work with a clock synchornization convention that's not Einsteinian. But perhaps I'm wrong about that.

Assuming that that is your motivation, though, as a matter of semantics I would say that momentum still exists as a conserved physical quantity, it's just no longer given by the relationship p=mv, but by some other relationship.

For any massive object, for instance, it's possible to define momentum in a relativistically correct manner as mass * proper velocity, where proper velocity is the distance an object moves (measured in a particular frame of reference) divided by the proper time takes for the object to move said distance. Note that this proper time interval does not depend on any frame of reference, as it's independent of the observer.

If the concept of proper velocity is unfamiliar, wiki has a short discussion of it <<link>>.

This won't work for calculating the momentum of light, but it will give the correct answer for momentum for any object moving slower than light, in a manner that's independent of any clock synchronization convention used. You didn't mention clock synchronization explicity, but of course it's the Einstein clock synchronziation convention that makes the speed of light the same in both directions.

It's routine to define the energy-momentum 4-vector as mass * proper velocity. And it's fairly routine to note that the energy momentum 4-vector contains the energy and the momentum 3-vector. So a lot of it is semantics and what one is used to.
Thanks for the reply. My motivation is that the notion of light not moving the same speed both ways violates my sense of symmetry and seems vaguely offensive for reasons I can’t explain. But if I understand what many have pointed out here it’s more or less a choice of coordinates.
 
  • #23
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the notion of light not moving the same speed both ways violates my sense of symmetry and seems vaguely offensive for reasons I can’t explain.
And you're in good company too.... I'd expect that most people will make a similar aesthetic judgment.
It just turns out that it's an aesthetic judgment about descriptions of the universe, not about the universe itself.
 
  • #24
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The fundamental truth is that light, in vacuum, follows null paths. That's a statement about geometry and completely independent of coordinates or frames or whatever. But how you choose to divide spacetime into space and time is up to you, and the projection of those null paths onto your choice of space depends on it.

If you choose to make your spatial "planes" orthogonal to your time direction then the paths are isotropic because the "planes" are symmetric under any rotation about the time axis. If you choose them to be non-orthogonal the paths are not isotropic because the "planes"
are no linger symmetric under rotation. Naturally, picking orthogonal planes is nicer.
 
  • #25
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Thanks for the reply. My motivation is that the notion of light not moving the same speed both ways violates my sense of symmetry and seems vaguely offensive for reasons I can’t explain. But if I understand what many have pointed out here it’s more or less a choice of coordinates.

Yes, it's a choice of time coordinates, in particular.

What may be annoying you about the choice of coordinates where the light speed is different in different directions is that the coordinates are aniosotropic (not the same in all directions), while the physics is istoropic.

It's usual in special relativity to restrict oneself to coordinates which respect the isotropy of physical laws. EInstein did that in his 1905 paper on special relativity, for instance. Tensor methods can handle strange choices of coordinates, including non-Einsteinian clock synchronization schemes, if one really needs to, but they don't really offer much physical insight.
 
  • #26
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We recently had a similar thread on this topic, but it was with respect to a crank's attempt to utilize this for religious purposes. The following question has nothing to do with that, but it could be related to it.

Basically, here's the deal: when we look at galaxies very, very far away, they all appear to be very young. This implies that light had to have taken a long time to reach us. If we could choose a coordinate system where their light got here instantaneously, wouldn't they appear as old as every other galaxy? Or in choosing such a synchronization convention, are we choosing a frame in which those galaxies just formed, and that is why they look so young?

https://imagine.gsfc.nasa.gov/features/cosmic/farthest_info.html

All these distant galaxies are viewed with light that was emitted around a few hundred years after the big bang (in the isotropic CMB frame), and all appear to be young when their light reaches our telescope. Why wouldn't they appear ancient if incoming light really traveled instantly to us? Or if we "chose" such a convention? Surely that is an argument against any arbitrary convention?


Or is it again simply choosing a frame where those galaxies really are that young?
 
  • #27
Ibix
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Or is it again simply choosing a frame where those galaxies really are that young?
This. The point is that "at the same time coordinate as you" is a concept that's up to you. You are free to define it any way you like, as long as you don't assign multiple coordinates to an event.

It would make sense to link it to something physical. That's what Einstein coordinates do in flat spacetime - they agree that two clocks are synchronised if they both literally see the other lagging by the same amount. That's also what FLRW coordinates do in an FLRW universe - here they pick observers who see the CMB as isotropic and who zeroed their clocks at the Big Bang singularity and define these clocks as synchronised.

But you don't have to do it. You can define anything you like as a time coordinate as long as it increases in a time-like direction. You will find that your notion of time usually doesn't correspond to anyone else's. You will also usually end up with more complex and opaque maths because you've sacrificed a direct correspondence between your core mathematical concepts and the physics. But if you want to do it, that's up to you.

An Earthbound example is latitude and longitude. Since the coordinate poles lie on the physical rotation axis, the coordinates are related to something physically meaningful and physically meaningful things (like the tropics and arctic circles) have simple representations. And since the magnetic field comes from the spin of the core we get a free way of measuring orientation relative to this coordinate system.

But we could pick anywhere on the Earth's surface as the coordinate pole. It's just a sphere. But it would be silly to do so because it's much harder to describe weather patterns (that are related to rotation) and compasses don't do anything relevant.
 
  • #28
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This. The point is that "at the same time coordinate as you" is a concept that's up to you. You are free to define it any way you like, as long as you don't assign multiple coordinates to an event.

It would make sense to link it to something physical. That's what Einstein coordinates do in flat spacetime - they agree that two clocks are synchronised if they both literally see the other lagging by the same amount. That's also what FLRW coordinates do in an FLRW universe - here they pick observers who see the CMB as isotropic and who zeroed their clocks at the Big Bang singularity and define these clocks as synchronised.

But you don't have to do it. You can define anything you like as a time coordinate as long as it increases in a time-like direction. You will find that your notion of time usually doesn't correspond to anyone else's. You will also usually end up with more complex and opaque maths because you've sacrificed a direct correspondence between your core mathematical concepts and the physics. But if you want to do it, that's up to you.

An Earthbound example is latitude and longitude. Since the coordinate poles lie on the physical rotation axis, the coordinates are related to something physically meaningful and physically meaningful things (like the tropics and arctic circles) have simple representations. And since the magnetic field comes from the spin of the core we get a free way of measuring orientation relative to this coordinate system.

But we could pick anywhere on the Earth's surface as the coordinate pole. It's just a sphere. But it would be silly to do so because it's much harder to describe weather patterns (that are related to rotation) and compasses don't do anything relevant.
But we cannot transform out differential aging, or even the fact that in every reference frame, all the galaxies should never appear to be the same age, unless that frame was equidistant from all of them (and surely no such frame exists). Am I right on that one? That is, we can use a convention to choose time coordinates where distant galaxies have just recently been born, but we can't choose one where the previous is true AND the nearer galaxies which appear older have also just recently been born (because in our frame they clearly are old, regardless of how fast we choose the incoming speed of light).
 
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  • #29
Ibix
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But we cannot transform out differential aging, or even the fact that in every reference frame, galaxies should never appear to be the same age, unless that frame was equidistant from all of them (and surely no such frame exists). Am I right on that one? That is, we can use a convention to choose time coordinates where distant galaxies have just recently been born, but we can't choose one where the previous is true AND the nearer galaxies which appear older have also just recently been born (because in our frame they clearly are old, regardless of how fast we choose the incoming speed of light).
Correct. If you look through a telescope at a co-moving clock then you see what you see - 12bn years since the Big Bang, for example. The FLRW explanation is that it's actually 1.9bn years away and light took 1.9bn years to get here, so the clock reads 13.9bn years now, same as ours. The explanation being touted in the other thread is that "now" is whatever the clocks appear to be reading to observers on Earth. So nearby clocks - for some reason - have been running longer than further away clocks. As long as you are willing to pay the mathematical and conceptual price of making that claim, that's fine.

The advantage to FLRW coordinates is that they reflect the symmetry of the physics. For example, any FLRW co-moving observer sees the universe looking the same (on cosmological scales) as any other when their own time-since-the-Big-Bang clock shows a specified time. Trivially, then, the owner of the clock in that distant galaxy will see our clock reading 12bn when his reads 13.9bn - because he's in the exact same situation as us. Using weird anisotropic coordinates completely obscures that. It's still true, but I would need a few hours and a symbolic maths package to prove it if I used the weird coordinates and didn't know a transform to the simple ones.
 

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