Derivation of the Equation for Relativistic Momentum

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SUMMARY

The equation for relativistic momentum is defined as p = γmv, where γ (gamma) represents the Lorentz factor, which accounts for time dilation and length contraction at relativistic speeds. The discussion emphasizes that relativistic mass is a misnomer and should be understood as the product of γ and proper mass m(0), which has no physical meaning. The derivation of relativistic momentum is linked to the need to reconcile it with Newtonian momentum, p = mv, and the concept of 4-momentum in special relativity. The gamma factor is essential for these definitions and reflects the relationship between energy and momentum in relativistic physics.

PREREQUISITES
  • Understanding of special relativity concepts, including Lorentz transformations.
  • Familiarity with the definition and implications of proper mass (m(0)).
  • Knowledge of the 4-momentum vector and its components.
  • Basic grasp of Newtonian mechanics for comparison with relativistic equations.
NEXT STEPS
  • Study the derivation of the Lorentz factor γ in special relativity.
  • Learn about the implications of 4-momentum in relativistic physics.
  • Explore the differences between relativistic and classical momentum through examples.
  • Investigate the historical context and evolution of the concept of relativistic mass.
USEFUL FOR

Students of physics, educators teaching special relativity, and researchers interested in the foundations of relativistic mechanics will benefit from this discussion.

NanakiXIII
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I asked a quite similar question about relativistic mass and the reason for this question is identical: I can't seem to dig up any derivation for the equation for relativistic momentum:

p=\gamma mv

If anyone could point me in the right direction, I'd much appreciate it.
 
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NanakiXIII said:
I asked a quite similar question about relativistic mass and the reason for this question is identical: I can't seem to dig up any derivation for the equation for relativistic momentum:

p=\gamma mv

If anyone could point me in the right direction, I'd much appreciate it.

Because this is a definition. And so is the relativistic total energy:


E=\gamma mc^2
 
I see. Why is it defined as such, exactly? There must be a reason for adding the so frequently seen gamma, no?

Another question on the side: I've seen two different versions of the equation for the mass-energy equivalence, one with and one without the gamma factor. What's the difference?
 
NanakiXIII said:
I see. Why is it defined as such, exactly? There must be a reason for adding the so frequently seen gamma, no?

I explained that to you in the other thread (relativisic mass) a few minutes ago.


Another question on the side: I've seen two different versions of the equation for the mass-energy equivalence, one with and one without the gamma factor. What's the difference?

Same reason as momentum, I also explained that to you in the other thread.
 
You mentioned the following:

nakurusil said:
The whole darned thing was introduced in order to reconcile the relativistic momentum/energy:

p=\gamma m(0)v (1)
E=\gamma m(0)c^2

with the Newtonian counterpart:p=mv (2)

So the best thing is to tell your teacher that your proof is you grouped together \gamma and proper mass m(0) into \gamma m(0) and you assigned that quantity to m

You mean the reason for the gamma is because of the use of relativistic mass? And yet in the other thread you tell me to base relativistic mass on relativistic momentum. That's circular. Are you saying that relativistic mass is a definition and thus relativistic momentum is as well? That would still leave the question of "why the gamma?".
 
NanakiXIII said:
You mentioned the following:



You mean the reason for the gamma is because of the use of relativistic mass? And yet in the other thread you tell me to base relativistic mass on relativistic momentum. That's circular.

"Relativistic mass" is just a misnomer, ok? Try to learn to forget about it, it has no meaning. Tolman's derivation from the other thread has no "relativistic momentum" in it, ok?


Are you saying that relativistic mass is a definition and thus relativistic momentum is as well? That would still leave the question of "why the gamma?".

Can't you read ? Relativistic momentum is a definition.
"Relativistic mass" is an unfortunate misnomer that corresponds to the result of multiplying \gamma by proper mass. It has no physical meaning.
 
Given the 4-momentum vector \tilde P,
an inertial observer (with unit 4-velocity \tilde t
can write that vector as the sum of two vectors, a "temporal" one parallel to \tilde t and a "spatial" one perpendicular to \tilde t.
\gamma is \cosh{\theta}, the analogue of cosine(angle) , and \gamma\beta is \sinh{\theta}, the analogue of sine(angle), where the [Minkowski-]angle \theta (called the rapidity) is between \tilde P and \tilde t.
 
NanakiXIII said:
I can't seem to dig up any derivation for the equation for relativistic momentum:

p=\gamma mv

There are some leads in this thread from last year:

https://www.physicsforums.com/showthread.php?t=107361

(which I should have thought of looking for when I posted in your other thread about relativistic mass)
 

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