Accelerating charged particle radiation reaction

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Discussion Overview

The discussion revolves around the radiation reaction of accelerating charged particles, particularly how the emission of electromagnetic waves affects the relationship between force, work, and kinetic energy. Participants explore the implications of this phenomenon on classical mechanics, specifically Newton's second law, and its application in various contexts such as antennas and particle accelerators.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that when a charged particle accelerates, it emits electromagnetic waves, implying that not all work done on the particle contributes to its kinetic energy, challenging the applicability of Newton's F=ma.
  • Others agree that while F=ma holds, it must account for forces from the electromagnetic field, suggesting that the effect of radiation reaction is negligible in many practical scenarios.
  • One participant argues against the notion of neglecting the radiation reaction, citing examples like antennas and the energy loss of a charged particle in orbit due to radiation.
  • There is a discussion about the applicability of F=ma in specific contexts, with some suggesting that more complex field equations are necessary for scenarios involving electromagnetic waves.
  • Another participant introduces the concept of using F=d(mv)/dt as a potential alternative to F=ma in certain situations.
  • The conversation touches on the unsolved nature of radiation reaction in classical electrodynamics, highlighting the complexities and peculiarities of point particles interacting with their own radiation fields.
  • A recommended source for further reading on this topic is the book "Classical Charged Particles" by F. Rohrlich.

Areas of Agreement / Disagreement

Participants express differing views on the significance of radiation reaction and its implications for classical mechanics. While some agree that F=ma can be modified to include electromagnetic effects, others challenge this perspective, leading to an unresolved discussion on the topic.

Contextual Notes

The discussion reveals limitations in applying classical mechanics to charged particles, particularly regarding the assumptions made about forces and energy conservation in electromagnetic contexts. The complexity of the interactions and the need for advanced equations are acknowledged but not resolved.

Who May Find This Useful

This discussion may be of interest to those studying classical electrodynamics, particle physics, or anyone exploring the implications of electromagnetic radiation on mechanical systems.

roboticmehdi
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It is known that if a charged particle accelerates then it emits electromagnetic wave (energy). If so then this means that the work we do on particle, W=F*s, doesn't all go to particles kinetic energy, E=0.5*m*v^2. Then this means that Newton's F=m*a doesn't hold for charged objects, particles, masses, etc.. Is that true? If yes, then what resists particle to accelerate to the speed it deserves ( F*s=0.5*m*v^2, solve for v ). I hope i could explain my point. I am sorry i ask a lot about electromagnetism but it is so damn confusing to me, i can't find peace if i don't understand it properly.
 
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hi roboticmehdi! :smile:

(try using the X2 button just above the Reply box :wink:)
roboticmehdi said:
… if a charged particle accelerates then it emits electromagnetic wave (energy). If so then this means that the work we do on particle, W=F*s, doesn't all go to particles kinetic energy, E=0.5*m*v^2. Then this means that Newton's F=m*a doesn't hold for charged objects, particles, masses, etc.. Is that true?

that's correct :smile:

some of the work goes into the electromagnetic field, whose energy density increases

F = ma still holds, but you have to include the force from the field!

however, the effect is negligible in practice … a lot less than the air resistance which we also usually ignore! :wink:
 
tiny-tim said:
hi roboticmehdi! :smile:

(try using the X2 button just above the Reply box :wink:)


that's correct :smile:

some of the work goes into the electromagnetic field, whose energy density increases

F = ma still holds, but you have to include the force from the field!

however, the effect is negligible in practice … a lot less than the air resistance which we also usually ignore! :wink:


Why negligible? i think it is not negligible, for example in antennas, which try to deliver as much work as possible to electromagnetic waves, and for example a negatively charged sphere orbiting positively charged sphere of much bigger mass, the orbiting sphere would eventually lose all of its orbit energy to electromagnetic waves. then there are particle accelerators and etc. anyway, thanks for reply. can you tell me more about this ? or give good sources? what is that force acting on a particle? how it works ? thank you.
 
roboticmehdi said:
i think it is not negligible, for example in antennas, which try to deliver as much work as possible to electromagnetic waves,

but we wouldn't use F = ma for an antenna …

what would be the body with mass m in that equation? :confused:
and for example a negatively charged sphere orbiting positively charged sphere of much bigger mass …

"orbiting"? how would that happen?
then there are particle accelerators

again, we don't use F = ma, we use more complicated field equations
 
tiny-tim said:
but we wouldn't use F = ma for an antenna …

what would be the body with mass m in that equation? :confused:

electrons are accelerated in antenna by electric field in the conductor. that electric field applies force on electron and it accelerates. electron has mass. so theoreticly it is possible to apply F=ma. to make things simpler you can assume the conductor to be a superconductor so that there is no resistance of wire to electrons. its like ignoring air resistance and making the environment airless, i.e. vacuum.


"orbiting"? how would that happen?

the same way as Earth orbits sun. the negatively charged sphere would be attracted to positively charged sphere. having the right initial velocity, it would circle around positively charged sphere. but of cource the orbit would decay and lose all energy to electromagnetic waves. the circling body would eventually fall on positively charged sphere.


again, we don't use F = ma, we use more complicated field equations

ok maybe not F=ma here but definitely F=d(mv)/dt
 
i don't how to do this sorry. in my upper post some of my comments are inside the quoted text. don't miss it.
 
anybody has other answers to my question ?
 
We don't typically use F = m a directly with electromagnetic waves, but it is still there in principle. We talk more in terms of energies than forces. The power radiated by an antenna, for instance, is not calculated as the force times velocity, but rather as the energy flow rate. The conservation of energy equation in electromagnetics accounts for both a force giving kinetic energy to a charged particle and also causing energy to radiate away.
 
This is a problem that is unsolved in classical electrodynamics. Classical point particles interacting with their own radiation field leads to equations with weird properties, predicting among other things self-acceleration.

The best source to learn about this difficult problem is the book

F. Rohrlich, Classical Charged Particles, World Scientific 2007
 

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