Conservation of momentum a universal truth

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Discussion Overview

The discussion centers around the concept of conservation of momentum, particularly in the context of relativistic physics. Participants explore the implications of momentum conservation across different frames of reference, the relationship between mass and momentum, and the effects of time dilation on these concepts.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that conservation of momentum is a universal truth, linking it to the mass equation m = m0/SQRT(1 - v2/c2) and suggesting that mass increases to conserve momentum in moving frames.
  • Others clarify that at everyday speeds, momentum simplifies to p = mv, and that time dilation affects processes on the moving body as seen from the rest frame, not the velocity itself.
  • Some participants argue that momentum is not invariant under Lorentz transformations, indicating that different observers will measure different values of momentum for the same event.
  • A practical example is presented involving meteorites colliding in space, illustrating that while momentum is conserved in each frame, the values differ across observers.
  • There is a discussion about the distinction between conservation and invariance, with some participants emphasizing that while momentum is conserved, it is not frame-invariant.
  • One participant questions the terminology of "relativistic mass" and its implications for momentum conservation, suggesting a need for clarity in definitions.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between momentum, mass, and frame of reference. There is no consensus on the implications of relativistic effects on momentum or the terminology used to describe these concepts.

Contextual Notes

Participants note that the discussion involves complex definitions and assumptions regarding relativistic mass, energy, and momentum, which may not be universally agreed upon. The nuances of frame invariance versus conservation are highlighted as a source of confusion.

  • #31
starthaus said:
This is a very nice post. Have you found a reference to the fact that m²c²=E²/c²-px²-py²-pz² holds for a system of particles also, not only for individual particles? I managed to prove it (the proof isn't trivial) but I haven't seen the proof in any book. (maybe in Griffiths' "Introduction to Particle Physics"? I don't have the book).

ETA: I found a proof in Rindler , pages 117-118. Takes him 1.5 pages of calculations to prove it. Interesting discussion on the fact that the total energy-momentum of the systm is not trivially a four-vector, one needs to sweat it out.

I like that m²c²=E²/c²-px²-py²-pz² - looks neat.

I looked this book up on Google Books and it got me to page 117 - just for grins - and that's just the start of the proof - The Zero Momentum Frame. The book is $97 somewhere. AbeBooks doesn't have it.

You're right... It isn't simple. We'll forgo that pleasure. I still like my old induction approach - if it's good for one, it's good for two, etc. all the way on up. I know that isn't right but at least I can conceptualize it. In AB French he sort of does an "induction" approach to justifying the concept verbally (no formal proof.) He uses the fact that the momenta are linearly related which allows for this "addition" or \sum concept. I have used that before when we studied vectors in ejection bailout systems for jet aircraft. If the three-space vectors are not linear, you cannot add them up and get a good answer. Had to use the numerical solutions of calculating each minute step along the way.

My son lives a few blocks from UT Texas Dallas where Wolfgang Rindler teaches and if I really needed it I could get him to go the llibrary there and Xerox those pages.
 
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  • #32
Is this the proof you saw in 2006 Rindler on page 117-18?

No way would I ever understand that. I would have to spend the last 50 years since high school getting it straight and even then wouldn't get it.

I'll accept the premise that one can find energy-momentum equations for systems of particles without understanding the proof.

The equation that DaleSpam gave (m²c²=E²/c²-px²-py²-pz²) is really another way of stating the AP French equation on page 213 of Special Relativity

-E02/c2 = px2 + py2 + pz2 + (iE/c)2

That's good enough for me.
 

Attachments

  • #33
stevmg said:
Is this the proof you saw in 2006 Rindler on page 117-18?

Yes.

No way would I ever understand that. I would have to spend the last 50 years since high school getting it straight and even then wouldn't get it.

No one said that physics is easy. I have a more direct proof than Rindler's but it isn't trivial by any stretch of imagination.

I'll accept the premise that one can find energy-momentum equations for systems of particles without understanding the proof.

This is a bad idea, we need to strive to understand the proofs. Otherwise, we become robots that plug in numbers into equations that we don't understand. Or worse, we use equations that do not apply.
 
  • #34
OK, but if it takes me 50 more years to understand it, I will give you the derivation in the old soldiers' home.

I will first read space-time physics and then maybe invest in Rindler.

The price we pay for our intellectual curiosity.
 

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