Relativistic centripetal force

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SUMMARY

The discussion centers on the derivation and understanding of the relativistic centripetal force, specifically expressed as F = mv^{2}/R[1-(v/c)^{2}]^{3/2}. Participants debate the implications of relativistic effects on measurements of force and acceleration, particularly in the context of a hypothetical scenario involving Superman spinning a ball at 90% the speed of light. Key points include the importance of frame of reference in measuring force and the distinction between proper time and lab time in relativistic calculations. The conversation highlights the necessity of dimensional analysis and the use of geometric units in relativistic physics.

PREREQUISITES
  • Understanding of relativistic physics concepts, including proper time and frame of reference.
  • Familiarity with centripetal force and its mathematical representation.
  • Knowledge of four-velocity and four-acceleration in the context of special relativity.
  • Proficiency in dimensional analysis and the implications of using geometric units.
NEXT STEPS
  • Study the derivation of relativistic centripetal force in detail.
  • Learn about the implications of proper time versus lab time in relativistic scenarios.
  • Explore the concept of four-acceleration and its calculation in special relativity.
  • Investigate the use of geometric units in physics and their advantages in simplifying equations.
USEFUL FOR

Physicists, students of relativity, and anyone interested in advanced mechanics, particularly those focusing on relativistic effects in circular motion.

  • #31
Rotation?

HallsofIvy said:
Do you remember that relativistic effect happen along the direction of motion?

What relativistic effect are you referring to?
 
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  • #32
malawi_glenn said:
the constant is 0.3*B, where B is measured in T, and p in GeV/c

Where is my suggested typo?

That forumula is widely used in particle physics.
Sorry, I misunderstood the question. It seems to me that you have two separate questions, though, if I'm understanding it correctly this time.

1) How do you compute the momentum of a particle, given its observed radius of curvature in a magnetic field of known strength. (You've supplied your own answer to this one, it looks right though I haven't double checked it)

2) What is the force (i.e. dp/dt) on that particle in the lab frame?

The answer gamma m v^2 / r is correct here as well with these assumptions.

Note that you have to specify a frame in order to ask what the 3-force is. One of the advantages of 4-forces is that they are geometric, frame-independent objects , but the magnitude of the 3-force definitely depends on the frame in which it is measured.
 
  • #33
pervect said:
Sorry, I misunderstood the question. It seems to me that you have two separate questions, though, if I'm understanding it correctly this time.

1) How do you compute the momentum of a particle, given its observed radius of curvature in a magnetic field of known strength. (You've supplied your own answer to this one, it looks right though I haven't double checked it)

2) What is the force (i.e. dp/dt) on that particle in the lab frame?

The answer gamma m v^2 / r is correct here as well with these assumptions.

Note that you have to specify a frame in order to ask what the 3-force is. One of the advantages of 4-forces is that they are geometric, frame-independent objects , but the magnitude of the 3-force definitely depends on the frame in which it is measured.

The thing is that I don't have a question, I just wanted to add what I obtained to this discussion.

Maybe I should have written "I WAS trying to derive this forumula.." And then I played a bit, and also searched in some books etc to werify my steps, that's all. And I wanted to contribute with my "research" in this thread, where to OP seemed to find the expression i posted.
 
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