Two Frames of 0-Momentum in the Minkowski Plane?

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Discussion Overview

The discussion centers around the concept of frames of reference with zero total momentum in Minkowski spacetime. Participants explore whether multiple frames can exist where the total momentum is zero, particularly in scenarios involving two non-accelerating masses moving in different directions. The conversation includes theoretical considerations and mathematical reasoning related to Lorentz transformations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions the uniqueness of the frame with zero total momentum, suggesting that two different methods yield different results for the direction of 2-velocities in Minkowski spacetime.
  • Another participant argues that unless the total energy is zero, there exists a unique frame where the total momentum is zero, providing a mathematical expression for determining the required relative speed between frames.
  • A third participant challenges the methods proposed by the first participant, suggesting that the total momenta should be added vectorially and then transformed using a specific velocity derived from the total momentum and energy.
  • The same participant acknowledges a mistake in their reasoning regarding the transformation process, specifically noting an oversight in rotating the velocity vectors to align in the x-direction.
  • Further clarification is made about the nature of the vectors involved in the transformation, correcting the earlier statement about the dimensionality of the vectors.

Areas of Agreement / Disagreement

Participants express differing views on the uniqueness of the zero momentum frame, with some asserting that it is unique under certain conditions while others suggest that multiple frames may exist. The discussion remains unresolved regarding the implications of these differing perspectives.

Contextual Notes

Participants highlight limitations in their methods, including assumptions about the direction of momentum and the need for proper vector rotation during Lorentz transformations. These factors contribute to the complexity of determining the zero momentum frame.

haruna
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Hello to everybody,

the question seems trivial in my mind, yet, is it legal to say that there is not unique frame of 0 total momentum in the Minkowski spacetime plane?

I am thinking of two non-accelerating equal masses on a horizontal plane, one is moving horizontally, the other perpendicularly as their respective 2-velocities in the Minkowski spacetime plane indicate. A quick way to find the frame of 0-momentum, one either moves along with the horizontal moving mass and Lorentz-transforms the velocity of the other mass, or does it by following the perpendicularly pointed mass.

These two separate methods yield two different results as to the direction of the respected 2-velocities of the masses in the Minkowski plane, very much unlike the Newtonian case where they're the same regardless.
So in this case, there must be two frames of 0-momentum. Is this legal to say, or they both cannot be told apart?
 
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Unless the total energy is zero, there is a unique frame in which the total momentum is zero. Suppose that in one frame, the total momentum is in the x-direction. Then in another frame, the momentum in the x-direction will be given by:

[itex]p' = \gamma (p - v E/c^2)[/itex]

where [itex]v[/itex] is the relative speed between the two frames (assuming the velocity is in the x-direction), and where [itex]E[/itex] is the total energy in the original frame and [itex]p[/itex] is the momentum. That equation uniquely determines the value of [itex]v[/itex] to make [itex]p'=0[/itex]: [itex]v = p c^2/E[/itex].

If the momentum is not in the x-direction, you can first perform a Lorentz transformation to get the momentum zero in the x-direction, then perform a second transformation to get it zero in the y-direction, then a third to get it zero in the z-direction. The resulting frame is uniquely determined by the momentum and energy in the initial frame.
 
haruna: Both your methods are wrong.
Add the two momenta vectorially so P=p1+p2, and E=e1+e2.
Then Lorentz transform with v=-P/E.
 
Meir Achuz said:
haruna: Both your methods are wrong.
Add the two momenta vectorially so P=p1+p2, and E=e1+e2.
Then Lorentz transform with v=-P/E.

Yes, thank you both. I can see my mistake now, tho not for the reason you've just pointed out.

You see, when i move along one of the two masses bringing its speed to a standstill, I add the momenta vectorially by transferring the one component of momentum to the other moving mass.

My mistake was when I Lorentz-transformed with v=-P/E, I forgot to rotate the velocity 2 or (3-vectors in general case) to point both in the x-direction. I forgot to rotate the Minkowski plane in the direction θ of v where v=tanhθ, and was left with the same velocity directions as before the transformation.
 
haruna said:
My mistake was when I Lorentz-transformed with v=-P/E, I forgot to rotate the velocity 2 or (3-vectors in general case) to point both in the x-direction.

Oops. This is not right! The correct statement is: I forgot to rotate the velocity 3 or (4-vectors in the general case) to point both in the x-direction.
 

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