Exploring Newton's Third Law in an Imaginary Magnetic Field

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Discussion Overview

The discussion revolves around the implications of Newton's third law in the context of a theoretical scenario involving a coil generating a magnetic field and a charged particle interacting with that field after the coil is switched off. Participants explore the nature of electromagnetic forces, field propagation, and the relationship between the coil and the particle.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant proposes a scenario where a charged particle experiences electromagnetic force from a magnetic field generated by a coil that has been switched off, questioning how this aligns with Newton's third law.
  • Another participant suggests that the term "propagates" may be more appropriate than "permeates" when discussing the magnetic field, and clarifies that Newton's third law holds locally for interactions between the particle and the electromagnetic field.
  • A later reply reiterates that Newton's third law applies to the interaction between the coil and the field when the pulse was generated, referencing Feynman's example of moving charges where forces are not always equal and opposite.
  • One participant argues that if the charge is within the radiated field from the magnet, it will experience an accelerating force and may radiate a new wave opposing the incoming wave.
  • Another participant contends that when the current is turned off, the charge will be affected by the electric field caused by the collapsing magnetic field, suggesting that this force reacts directly on the magnet without propagation delay.

Areas of Agreement / Disagreement

Participants express differing views on the implications of electromagnetic interactions and the application of Newton's third law in this context. No consensus is reached regarding the nature of the forces involved or the timing of their effects.

Contextual Notes

Participants discuss the nuances of electromagnetic field interactions, including the distinction between radiated fields and induction fields, as well as the implications of field propagation and the timing of forces experienced by the charged particle.

pays_fan
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Hi, here's a theoretical problem that I am trying to find a satisfactory answer for.

Imagine a coil that is temporarily switched on an off and generates a magnetic field that permeates through space. Now imagine a charged particle passing through this field, at time that the coil is already switched off, and experiencing electromagnetic force. I would assume that the coil would not experience a reactive force because it is switched off (or for the sake of argumentation, it can even be disassembled by the time the charged particle experiences the magnetic field). How is this in line with Netwon's third law?
 
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pays_fan said:
a magnetic field that permeates through space
The word ”propagates” would probably be a better fit for what you want to say here. To permeate can also be taken to mean to exist everywhere.

If I understand your question correctly, you want to consider the a field pulse that propagates outwards and is of finite extent in time.

In an interaction with the electromagnetic field, Newton’s third law holds locally for the interaction between the paricle and the field itself. The electromagnetic field carries energy and momentum. This is described by the electromagnetic stress energy tensor. Newton’s third law also holds for the interaction between the coil and the field when the pulse was generated.
 
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Orodruin said:
In an interaction with the electromagnetic field, Newton’s third law holds locally for the interaction between the particle and the field itself. The electromagnetic field carries energy and momentum. This is described by the electromagnetic stress energy tensor. Newton’s third law also holds for the interaction between the coil and the field when the pulse was generated.
Yes, Feynman showed an example in his Lectures on Physics Volume II page 26-5 fig 26-6 that two charged particles can move in such a way that their forces are not always equal and opposite.
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Fig. 26–6. The forces between two moving charges are not always equal and opposite. It appears that “action” is not equal to “reaction.”

https://www.feynmanlectures.caltech.edu/II_26.html
 
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If the charge is in the radiated field from the magnet then it will experience an accelerating force. It seems to me that it will radiate a new wave opposing the incoming wave, in the manner of a conductor.
 
Radiation by the magnet implies that the magnet has a finite length. If the charge is very close to such a magnet, it will primarily experience the induction field of the magnet and so it is different to the case for the radiation field. When the current is turned off, the charge will now be in the E field caused by the collapsing magnetic field, and will experience a force. As far as I can see, this force will react directly on the magnet with zero propagation delay.
 

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