Does charge change with velocity?

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Discussion Overview

The discussion revolves around the effects of velocity on the charge and electromagnetic fields of charged particles, particularly in the context of special relativity. Participants explore concepts such as Lorentz contraction, the invariance of Maxwell's equations, and the implications for understanding electromagnetic forces and gravitational effects at relativistic speeds.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants propose that while mass appears to increase for an object moving close to the speed of light, the charge strength remains invariant as observed from another frame of reference.
  • Others argue that the electromagnetic field of a charged particle in motion undergoes Lorentz contraction, which affects the field's shape and strength in different directions.
  • A participant suggests an alternative explanation where the charge field's magnitude changes due to relativistic effects, rather than relying solely on Lorentz contraction.
  • Another viewpoint emphasizes that the concept of relativistic mass should be abandoned in favor of focusing on energy and momentum, as mass does not change with velocity.
  • One participant raises a question about the gravitational implications of relativistic mass for distant galaxies, expressing uncertainty about how general relativity addresses these concepts.
  • Several participants express confusion and seek clarification on the relationship between charge, mass, and relativistic effects, indicating a lack of consensus on these complex ideas.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether charge changes with velocity or how to interpret the implications of relativistic effects on electromagnetic fields. Multiple competing views remain, particularly regarding the concepts of charge density, relativistic mass, and the interpretation of experimental results.

Contextual Notes

Limitations include unresolved assumptions about the nature of charge and mass in relativistic contexts, as well as the dependence on definitions of charge density and electromagnetic fields. The discussion also reflects varying interpretations of experimental evidence related to Lorentz contraction and relativistic effects.

Who May Find This Useful

This discussion may be of interest to those studying special relativity, electromagnetism, or general relativity, as well as individuals curious about the implications of relativistic effects on physical concepts.

duordi
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If object A travels close to light speed of light with respect to object B then object A will seem to have an increased mass as observed by B.

If A is also a charged particle will the charge strength be increased also or will it remain at its rest velocity field strength as determined by B?
 
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No. In fact one reason why length, time, etc. change with speed is to make sure that Maxwell's equations are "invariant" under change from one inertial frame of reference to another- and Maxwell's equation govern electromagnetic field strength.
 
Shoot! every time I think I am starting to understand this stuff it throws me a curve.

Does a field of a charged particle in motion have a Lorenz contraction?
 
duordi said:
Shoot! every time I think I am starting to understand this stuff it throws me a curve.

Does a field of a charged particle in motion have a Lorenz contraction?
Yes, and this is actually very useful in understanding why there must be a magnetic force if electric charge is the same in every frame. If you want to better understand the relation between electromagnetism and relativity I recommend looking at this page (especially all the useful diagrams), which is adapted from a similar discussion in Purcell's undergraduate textbook Electricity and Magnetism.
 
I read the material and it all makes sense but it occurred to me you could explain the test charge response and the charges in the wire by replacing the Lorenz contraction with change in field charge magnitude due to a relativistic effects of a “charge in motion” principle.

That is to say instead of the moving charges being closer together with the same field strength, the charges are the same distance apart and the strength of the charges are increased.

The second thing I noted was that the charge field changes shape ( Lorenz contracts) when in motion.
So if a motionless charged particle A field strength is measured
and then the observer is accelerate to a velocity V, the field of A will contract in the direction of motion causing the field to weaken in the direction of motion and strengthen in a direction perpendicular to the direction of motion.

It would seem that a charged particle is similar to rest mass with gravity,
and that magnetic fields are similar to relativistic mass.

I assume this line of reasoning has been followed before and that it breaks down somewhere.

PS. I really enjoyed the reference material.
 
duordi said:
I read the material and it all makes sense but it occurred to me you could explain the test charge response and the charges in the wire by replacing the Lorenz contraction with change in field charge magnitude due to a relativistic effects of a “charge in motion” principle.

That is to say instead of the moving charges being closer together with the same field strength, the charges are the same distance apart and the strength of the charges are increased.

The second thing I noted was that the charge field changes shape ( Lorenz contracts) when in motion.
So if a motionless charged particle A field strength is measured
and then the observer is accelerate to a velocity V, the field of A will contract in the direction of motion causing the field to weaken in the direction of motion and strengthen in a direction perpendicular to the direction of motion.

It would seem that a charged particle is similar to rest mass with gravity,
and that magnetic fields are similar to relativistic mass.

I assume this line of reasoning has been followed before and that it breaks down somewhere.

PS. I really enjoyed the reference material.
Actually, that "line of reasoning" does not break down, but was contradicted by experiment. This was in fact Lorentz' theory to explain the null result of the Michaelson-Morley experiment: that the force of moving electrons strengthened just enough to "contract" one arm of the equipment as given by Lorentz' equation. It was a variation of The Michaelson-Morley experiment, Kennedy's experiment, that show that was NOT the case, leading to Einstein's theory that it was not just the material in the arm that contracted but space itself.
 
Also, this kind of directional dependence that you have noticed is another reason to drop the concept of relativistic mass. Don't think of mass as increasing relativistically either, just the energy and momentum.
 
The reason I was interested in relativistic mass is simple.

I was trying to determine if distant galaxies which are receding from us at a high velocity have a relativistic mass component causing an increase in the gravitational force they have on us.

GR does not have force equations only tidal fields and I do not know how to change this to something I can relate to in the real world, like a force or acceleration.

Newton’s equations do not work for near light speed velocities. .

Has the solution of this question already been completed with GR?

I am not capable to solve the GR equations.
Some day I hope to be able to solve GR equations, but until then I keep my interest alive by asking questions and learning as I go.
 
duordi said:
Shoot! every time I think I am starting to understand this stuff it throws me a curve.

Does a field of a charged particle in motion have a Lorenz contraction?

It is in fact the very fundamental Space-Time which we're living in that changes with Lorentz transformation, so everything relates to length, time, velocity...changes, but as one apple is still transformed into one apple, the charge of a particle will not change, although the charge density will. Mass doesn't change either, if not so, you'd be able to make a remote galaxy collapse just by moving yourself around!
 

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