How Does Relativistic Two-Way Momentum Appear to Different Observers?

In summary, momentum is a frame-variant quantity and different observers will generally disagree on its value. This has always been true, even in Newtonian physics. In special relativity, a 4-dimensional vector is used to describe momentum and its components change in the same way as the coordinates change when changing frames of reference. However, there are arguments for defining 4-momentum as a covector, but this is not necessary for understanding the concept of momentum. It is important to note that simply because two frames disagree about the value of momentum, it does not make one frame more correct than the other. Momentum is conserved and works exactly as it should in each frame of reference.
  • #36
lugita15 said:
I think you mean the same direction; in frame S1 initially ball A is moving to the right at 1m/s, and it collides elastically with the stationary ball B, so then ball A comes to a stop and ball B moves to the right at 1m/s. Now consider frame S2, which is moving at 3m/s to the left with respect to frame S1. In frame S2 initially ball A is moving at 4m/s to the right and ball B is moving at 3m/s to the right, and they collide elastically, so then ball A is moving at 3m/s to the right and ball B is moving at 4m/s to the right.

I meant the opposite side of the ball. So then how did you find that an object traveling at 4m/s would only transfer 1 Newton to the other object that is traveling at 3m/s?
 
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  • #37
John232 said:
Newton hits a bowling ball that weights 1kg with another bowling ball that weights 1kg. One is at rest on a table, and the other is moveing at 1 m/s. The ball at rest then gets hit and then moves 1m/s in the opposite direction.
Since you didn't work the problem out you made a mistake. The other ball will move in the same direction as the original ball. But anyway, consider the frame where the other ball is at initially at rest.

One ball is moving at -1 m/s and is on a table which is also moving at -1 m/s, the other ball is at rest. The ball at rest gets hit and then moves at -1 m/s.

EDIT: lugita15's analysis also works (and is more interesting), the point is that you can use any frame you feel like using.
 
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  • #38
John232 said:
I meant the opposite side of the ball. So then how did you find that an object traveling at 4m/s would only transfer 1 Newton to the other object that is traveling at 3m/s?
They're transferring momentum, measured in kg m/s, not force, measured in kg m/s^2 or Newtons (although they presumably will exert forces on each other while they are colliding). The momentum transferred between the two balls is (1 kg)(4m/s)-(1 kg)(3m/s) = 1 kg m/s.
 
  • #39
lugita15 said:
They're transferring momentum, measured in kg m/s, not force, measured in kg m/s^2 or Newtons (although they presumably will exert forces on each other while they are colliding). The momentum transferred between the two balls is (1 kg)(4m/s)-(1 kg)(3m/s) = 1 kg m/s.

Sounds a lot like what I was saying before. You have to find the difference in the two objects themselves to find the true transfer of momentum. That is what you just did by doing that calculation.
 
  • #40
John232 said:
Sounds a lot like what I was saying before. You have to find the difference in the two objects themselves to find the true transfer of momentum. That is what you just did by doing that calculation.
Didn't I just cover this in post #28?
 
  • #41
lugita15 said:
Didn't I just cover this in post #28?

I thought I did in my quote on post #28. I didn't see anything in the posted link that would show it would be used in a tranfer of momentum. It simply doesn't have some key variables in it to determine that. I think if it was used to determine a transfer of momentum by adding the velocities in this way it wouldn't give the correct value that an observer would get being at rest relative to one of the two objects. The addition of velocity formula in SR wouldn't be used to determine the transfer of momentum because the added distance between two objects is arbritray to the calculation. The two objects would be hitting each other not moveing away from each other closer to the speed of light.
 
  • #42
John232 said:
I think if it was used to determine a transfer of momentum by adding the velocities in this way it wouldn't give the correct value that an observer would get being at rest relative to one of the two objects. The addition of velocity formula in SR wouldn't be used to determine the transfer of momentum because the added distance between two objects is arbritray to the calculation. The two objects would be hitting each other not moveing away from each other closer to the speed of light.
In SR it is actually more convenient to work with momentum than with velocity. Momentum adds like normal in SR, and it is only the relationship between momentum and velocity which is non-linear. The conservation of the 4-momentum encapsulates the conservation of energy, conservation of mass, and conservation of momentum into one nice convenient mathematical package.
 
  • #43
John232 said:
I meant the opposite side of the ball. So then how did you find that an object traveling at 4m/s would only transfer 1 Newton to the other object that is traveling at 3m/s?
The same way you found it in the original. Conservation of KE for an elastic collision.
 
  • #44
It doesn't seem like it would be that convenient to work to me.

I got Ʃ F = m1(v1'-v1°)/(t√(1-(v1'+v1°)^2/4c^2) + m2(v2'-v2°)/(t√(1-(v2'+v2°)^2/4c^2)
 
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  • #45
Use the four-momentum instead. That is what I was referring to above.
 
  • #46
DaleSpam said:
Use the four-momentum instead. That is what I was referring to above.

I would but I wouldn't even know what to put into that thing. I figured if you found one dimension you would have them all. What is a U^μ? The collision i gave was two vectors coming at each other, different velocities would have different vectors.
 
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