Mass of a system of two photons

In summary, the mass of a system of two photons is an invariant and it depends on the reference frame in which it is observed. When the photons are moving in opposite directions, the mass of the system is always 2E_0, where E_0 is the energy of the photons in the frame where the momentum is zero. In a different frame, the mass can be calculated using the relativistic doppler shift factor, but it will always be an invariant. The confusion around this topic may stem from confusion between the momentum of the system and the momenta of the individual photons.
  • #36
mass of two photons

Meir Achuz said:
It is not a paradox. It would just be that you made a mistake in the transformation. If done correctly, M^2 is invariant.
Thanks. You are right. Did you see the problem treated somewhere in the literature (the problem of two photons detected from different inertial reference frames in relative motion)?
 
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  • #37
Chris Hillman said:
...the distinction between momentum of a system of two particles and the momenta of the individual particles.

I'm not sure I see the distinction; surely the 4-momentum of a system of particles is simply the sum of the 4-momenta of the particles that make up the system?

If this is the case, then what is the distinction between the two?

If this is not the case, then why isn't it? And what is incorrect?
 
  • #38
masudr said:
I'm not sure I see the distinction; surely the 4-momentum of a system of particles is simply the sum of the 4-momenta of the particles that make up the system?

If this is the case, then what is the distinction between the two?

If this is not the case, then why isn't it? And what is incorrect?
Addition of two 4-vectors in a Minkowski spacetime often produce an unintuitive result. Each separate photon has no mass, but in some cases a system of photons does have mass. Localizing that mass is an entirely different but very interesting question.

One thing to keep in mind is that relativity is a classical theory. I think relativity theory really does not model photons very well. This is even more obvious in general relativity. Einstein, unlike Weyl was never comfortable with modeling matter in terms of complex wave mechanics.
 
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  • #39
MeJennifer said:
Addition of two 4-vectors in a Minkowski spacetime often produce an unintuitive result.

Is there or isn't there a distinction? And if so, then what is it?
 
  • #40
masudr said:
Is there or isn't there a distinction? And if so, then what is it?
They are different.

In case of two photons going in opposite directions each one has an individual mass of 0. But when you add both photons together you get something like 0 + 0 > 0. This is due to the non-Euclidean metric of spacetime.
 
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  • #41
mass of two photons

MeJennifer said:
They are different.

In case of two photons going in opposite directions each has one has an individual mass of 0. But when you add both photons together you get something like 0 + 0 > 0. The reason is related to the metric of spacetime.

Has that fact some influence on the discussion about the opportunity to use the concept of relativistic mass. That is only a question and not a statement! Thanks for the answer.
 
  • #42
Bernhard.Rubinstein said:
Has that fact some influence on the discussion about the opportunity to use the concept of relativistic mass. That is only a question and not a statement! Thanks for the answer.
I would think so.

Personally I do not agree with this "grand objection" expressed by the prevailing winds here on PF against the usage of relativistic mass. In the end it is simply a matter of terminology. As long as one understands the difference between relativistic and proper mass I see no issue.
 
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  • #43
Addition of two 4-vectors in a Minkowski spacetime often produce an unintuitive result. Each separate photon has no mass, but in some cases a system of photons does have mass.

Energy of a system of particles is a sum of particles' energies, and the momentum is also a sum of the momentums. But the mass of the system is not a sum of the masses of the particles. Since [tex]m^2=p_\mu p^\mu[/tex], thinking with four-vectors, this is nearly equivalent to saying that a norm of a sum of vectors is not a sum of the norms. That is, [tex]||x+y||\neq ||x||+||y||[/tex] in general. I don't think this is unintuitive. Improve your intuition on the matter :wink:

The inequality [tex]0+0>0[/tex] doesn't seem very related to this matter. You are not supposed to add masses, or other norms of vectors, in the first place.
 
  • #44
jostpuur said:
Energy of a system of particles is a sum of particles' energies, and the momentum is also a sum of the momentums.
Note that energy and momentum are not Lorentz invariant properties, instead they are covariant.
 
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  • #45
Time to lock this thread?

masudr said:
I'm not sure I see the distinction; surely the 4-momentum of a system of particles is simply the sum of the 4-momenta of the particles that make up the system?

If this is the case, then what is the distinction between the two?

If this is not the case, then why isn't it? And what is incorrect?

This thread was always terribly confused, and unfortunately it seems that my half-hearted attempt to nudge in a more fruitful direction failed. In fact, although some participants are in my "ignore list", I have the impression it has descended even further into the murk since my own contribution. Masudr, you must have misunderstood what I tried to tell someone (I don't remember the circumstances of the post you quoted), but I don't think it would be worthwhile to pursue this, given the degree of confusion in this thread.
 
  • #46
lightarrow said:
Of course I recognize it! My problem was I didn't recognize that mass IS NOT additive, that is, m1 + m2 IS NOT equal to the mass of the system.
Yep. I seemed very clear to me that you recognize that fact. The sum of the invariant masses is not additive, only the sum of the inertial (aka relativistic mass) is additive (and conserved). This conservation can be proved with no use of the conservation of energy, All that is required is that momentum is conserved in all inertial frames.

Pete
 
  • #47
mass of two photons

pmb_phy said:
Yep. I seemed very clear to me that you recognize that fact. The sum of the invariant masses is not additive, only the sum of the inertial (aka relativistic mass) is additive (and conserved). This conservation can be proved with no use of the conservation of energy, All that is required is that momentum is conserved in all inertial frames.

Pete
Please let me know how "all that is required is that momentum is conserved in all inertial frames." Your answer shows again that not using the concept of relativistic mass some confusion can arrise.:smile:
Thanks

Bernhard
 
  • #48
MeJennifer said:
Personally I do not agree with this "grand objection" expressed by the prevailing winds here on PF against the usage of relativistic mass. In the end it is simply a matter of terminology. As long as one understands the difference between relativistic and proper mass I see no issue.

reading this is refreshing (to me, at least).
 
  • #49
mass

rbj said:
reading this is refreshing (to me, at least).
for me too
 
  • #50
bernhard.rothenstein said:
Please let me know how "all that is required is that momentum is conserved in all inertial frames." Your answer shows again that not using the concept of relativistic mass some confusion can arrise.:smile:
Thanks

Bernhard
you can find the derivation on y we site at

http://www.geocities.com/physics_world/sr/conservation_of_mass.htm

Best wishes Bernhard

Pete
 
  • #51
MeJennifer said:
Note that energy and momentum are not Lorentz invariant properties, instead they are covariant.
Yay for MJ. :smile:

Not too many people know of that use of the term "covariant." Bravo to MJ :smile:

Pete
 
  • #52
rbj said:
reading this is refreshing (to me, at least).
Me too.

Pete
 
  • #53
MeJennifer said:
Note that energy and momentum are not Lorentz invariant properties, instead they are covariant.

Has anyone ever claimed anything contrary to that?
 

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