Contradiction in Abraham-Lorentz Force?

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Discussion Overview

The discussion revolves around the Abraham-Lorentz force and its implications for energy conservation when a charged particle is subjected to a constant force. Participants explore the relationship between force, acceleration, radiation, and energy, questioning whether the formula leads to contradictions regarding energy expenditure and radiation emission.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • One participant questions the implications of the Abraham-Lorentz force, suggesting that if a charge is pulled with a constant force, it would radiate energy without any recoil, potentially creating an infinite energy source.
  • Another participant challenges this reasoning by stating that if a photon is emitted, it would cause a recoil that changes the resultant force, implying a non-zero jerk and complicating the application of F = ma.
  • A different viewpoint suggests that the Abraham-Lorentz force is a result of the action on the charge, likening it to "emission friction," and questions how a constant force can lead to radiation without an opposing force to balance it.
  • Some participants assert that work is done on the kinetic energy of the charge, which appears to be separate from the energy radiated, indicating that the work-energy theorem applies.
  • References to academic papers are made, with one participant noting that energy for radiation may come from the fields surrounding the particle, but another questions the validity of this claim and its implications for Newton's third law.
  • Concerns are raised about the clarity of explanations regarding energy conservation and whether there is a contradiction in the understanding of the Abraham-Lorentz force and radiation energy.

Areas of Agreement / Disagreement

Participants express differing views on the implications of the Abraham-Lorentz force, with no consensus reached on whether the formula leads to contradictions regarding energy conservation. Multiple competing interpretations of the relationship between force, acceleration, and radiation remain unresolved.

Contextual Notes

Participants highlight limitations in the current understanding, including assumptions about constant force application, the nature of radiation emission, and the relationship between kinetic energy and radiated energy. There is also mention of unresolved mathematical steps and the dependence on definitions related to the forces involved.

Ozgen Eren
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Hey guys,

This is my fist post and I am curious enough about this to get a new account. Go on wikipedia for the formula and derivation of the abraham lorentz force: http://en.wikipedia.org/wiki/Abraham–Lorentz_force

Anyway my question is as follows:

Lets consider a charge that I am pulling with a constant force F.
Then obviously by F = ma it has a constant acceleration.
Thus it is radiating some energy.
But according to Abraham-Lorentz force there is no recoil force on the particle, so I spend no energy for radiation.

Because if this was the case I would just take a charge, pull it with a constant acceleration, harvest all the radiating energy, and then absorb the kinetic energy I just applied, and do it again and again. It would be my pretty little infinite energy source. Doesnt that imply any harmonic motion spreads infinite energy?

What is wrong, is it the formula or is it my reasoning?
 
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Ozgen Eren said:
Hey guys,

This is my fist post and I am curious enough about this to get a new account. Go on wikipedia for the formula and derivation of the abraham lorentz force: http://en.wikipedia.org/wiki/Abraham–Lorentz_force

Anyway my question is as follows:

Lets consider a charge that I am pulling with a constant force F.
Then obviously by F = ma it has a constant acceleration.
Thus it is radiating some energy.
But according to Abraham-Lorentz force there is no recoil force on the particle, so I spend no energy for radiation.

Because if this was the case I would just take a charge, pull it with a constant acceleration, harvest all the radiating energy, and then absorb the kinetic energy I just applied, and do it again and again. It would be my pretty little infinite energy source. Doesnt that imply any harmonic motion spreads infinite energy?

What is wrong, is it the formula or is it my reasoning?
How are you keeping the (resultant) force constant? If the particle emits a photon then it will recoil, and the resultant force will change over a very short period, giving a non-zero jerk. The Abraham-Lorentz force is a result of the emission, not the cause of it.
 
I didn't mean Abraham Lorentz force causes emission, I know its a result of our action upon the charge. I try to think of it as an "emission friction" if that's the right way to put it.

Vagn said:
the resultant force will change over a very short period, giving a non-zero jerk

So you suggest that instead of creating an opposite force to balance emission energy, it creates a non-zero jerk which corresponds to a derivative of force on F=ma. That actually makes sense but still the original formula don't seem like supporting it.

If we just apply a constant force to a charge, the derivative of acceleration will be zero as long as F=ma is valid. So no Abraham-Lorentz force, but emission. Thats what I am trying to understand.
 
If you are moving the charge with uniform acceleration ( though inverse square fields produce non uniform acceleration), you are doing some work as dictated by work energy theorem, that is appearing as radiation energy.. I see no paradox
 
Ozgen Eren said:
I didn't mean Abraham Lorentz force causes emission, I know its a result of our action upon the charge. I try to think of it as an "emission friction" if that's the right way to put it.
So you suggest that instead of creating an opposite force to balance emission energy, it creates a non-zero jerk which corresponds to a derivative of force on F=ma. That actually makes sense but still the original formula don't seem like supporting it.

If we just apply a constant acceleration to a charge, the derivative of acceleration will be zero as long as F=ma is valid. So no Abraham-Lorentz force, but emission. Thats what I am trying to understand.
The paper below discusses how to resolve the problem.
http://dx.doi.org/10.1016/0003-4916(60)90105-6
 
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Ehsan Farooq said:
If you are moving the charge with uniform acceleration ( though inverse square fields produce non uniform acceleration), you are doing some work as dictated by work energy theorem, that is appearing as radiation energy.. I see no paradox

No the work is done upon the kinetic energy, not upon the radiation. So what you applied = 1/2*m*V*V, what seems to exist : 1/2*m*V*V + Eradiation.

Vagn said:
Fulton, T., & Rohrlich, F. (1960). Classical radiation from a uniformly accelerated charge. Annals of Physics, 9(4), 499-517

I will take a look on that one, thanks.
 
Vagn said:
The paper below discusses how to resolve the problem.
http://dx.doi.org/10.1016/0003-4916(60)90105-6

Well I didn't buy the original article but found a free one which refers to it and restates the explanation. Here is the link:

http://users.jyu.fi/~ilsamaki/radiation.pdf

saying the following in summary:
"so it would seem the energy needed for the radiation is somehow supplied from the near part of the fields surrounding the particle."
Do you really think that is possible? It seemed too vague to me. There is no actual proof that it comes from its own field, its just a claim which would violate Newtons third law in the first place.

Plus electromagnetic waves travel with the speed of light. So even if it were to be effected by its own field, it could never have catched its own field after the instant the field is created. And we cannot suggest it is influenced by its own field at the very instant the field is created, because then it should have been influenced by its own fields in all directions, which would again result in zero net force.

Does someone knows a solid explanation for the energy conservation? I just want to know if there is a plain contradiction or a complete explanation.
 
Last edited by a moderator:

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