Can Momentum Exist Without Net Velocity in Special Relativity?

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SUMMARY

The discussion centers on the relationship between momentum and average velocity in the context of Special Relativity (SR). A user questions whether an asymmetric system can possess momentum while having zero net velocity, using a scenario involving N + 1 identical particles. The calculations reveal that total relativistic momentum can be non-zero despite no net movement. Key insights include the importance of energy transfer in momentum calculations and the distinction between intensive and extensive properties, with references to the Lorentz factor and the concept of "hidden momentum" in classical electrodynamics.

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  • Understanding of Special Relativity and the Lorentz factor
  • Basic knowledge of momentum and its relationship to velocity
  • Familiarity with intensive vs. extensive properties in physics
  • Concept of energy transfer in particle systems
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  • Research the implications of the Lorentz factor in relativistic momentum calculations
  • Explore the concept of "hidden momentum" in classical electrodynamics
  • Study the differences between intensive and extensive properties in physics
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Physicists, students of Special Relativity, and anyone interested in the nuances of momentum and velocity in relativistic systems.

Andy Bloch
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(I hope this post doesn't cross the border into the forbidden realm of quackery and speculation.) I have what seems like a simple question about Special Relativity but I haven’t seen it discussed anywhere, nor has anyone I've asked.

Does the nonlinearity of the Lorentz factor provide a way for an asymmetric system to have momentum with zero average velocity, and vice-versa?

Consider this example:
nparticles.png

There are N + 1 identical particles in this system. At any time, there is one particle (an electron, perhaps) moving to the left with relativistic velocity v (relative to the laboratory frame), and N particles moving to the right with velocity v/N. The process can be repeated continuously. There is no net movement of the system. But, it seems that the total (relativistic) momentum is non-zero. The total momentum to the left is (assuming v/N << c):

ptotal = γ m v - N m v / N = (γ-1) m v

where γ is the Lorentz factor.

Is there something I am missing?

Yes, I've ignored the periods of acceleration. But (1) if the clock hypothesis is true, making those periods very short should make any effect negligible, and (2) if the acceleration periods did affect the total momentum and exactly canceled it out, then changing the acceleration curve would have to have no effect on the total momentum. That doesn't seem likely to me.

(No, this would not seem to be a good way to power a spacecraft . It does not provide a constant thrust, just an initial velocity boost. I've done some calculations, with very generous assumptions, that suggest that even a velocity on the order of 1 m/s would not currently be feasible.)

I'm hoping someone here can quickly show me what is wrong with my math or reasoning, or provide a reference where this has been discussed.

Thanks in advance for any feedback.
 

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What do you mean by ”average velocity”? Velocity is an intensive property, not an extensive one.
 
How are you stopping the particles and turning them round? Have you accounted for the momentum transfer inherent in that?
 
Ibix said:
How are you stopping the particles and turning them round? Have you accounted for the momentum transfer inherent in that?
The amount of momentum transfer when accelerating a particle is the same as decelerating it back to zero velocity, but in opposite directions, so there should be no net momentum transfer.
 
Orodruin said:
What do you mean by ”average velocity”? Velocity is an intensive property, not an extensive one.
I probably should have written "net movement" instead of "average velocity."
 
Andy Bloch said:
The amount of momentum transfer when accelerating a particle is the same as decelerating it back to zero velocity, but in opposite directions, so there should be no net momentum transfer.
The key word there is "net". You need to get the energy absorbed in slowing the particle at one end up to the other end to accelerate the next one. And the mechanism that does that will carry momentum - presumably exactly enough to correct for your imbalance.
 
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Say Train whose mass is M kg, goes 1m/s and a passenger whose mass is m kg, is running -1m/s in the system of station. Average velocity of the two is zero but total momentum is (M-m)*1 kg m/s. I am sorry for this word trick.
 
Last edited:
Andy Bloch said:
I probably should have written "net movement" instead of "average velocity."

In classical physics, momentum is linearly proportional to velocity. So, in a system of particles of equal mass, the net momentum is zero iff the net velocity is zero. By this, I mean simply adding the velocity vectors for each particle.

In SR, momentum is no longer linearly proportional to velocity. In a system of particles of equal mass with zero net momentum, typically the net velocity is not zero.

You've essentially found this yourself through your calculations. There's no mystery as far as I can see.
 
There is no reasonable way of defining ”net movement” other than movement of the center of energy. This is given by the net momentum divided by the total energy. If the net momentum is zero so is the movement of the center of energy (for a closed system). It makes no sense whatsoever to define net movement by summing particle velocities. Again, velocity is intensive, not extensive. The extrnsive properties are energy and momentum.
 
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Ibix said:
The key word there is "net". You need to get the energy absorbed in slowing the particle at one end up to the other end to accelerate the next one. And the mechanism that does that will carry momentum - presumably exactly enough to correct for your imbalance.
This was the most helpful answer. Yes, transferring the energy back to the other end will offset the momentum difference.
 
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Google "hidden momentum". This concept is well-known in classical electrodynamics, though rather controversial.

Eugene.
 

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