Ampère force law, action, reaction

Click For Summary

Discussion Overview

The discussion revolves around the Ampère force law and its implications for Newton's third law in the context of electromagnetism. Participants explore the conditions under which the force law applies, the role of electromagnetic fields, and the relationship between current elements and fundamental physics. The scope includes theoretical considerations and potential applications in magnetohydrodynamics (MHD).

Discussion Character

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

Main Points Raised

  • One participant notes that the Ampère law does not balance action and reaction forces as expressed in the equation, raising questions about its interpretation.
  • Another participant argues that the force law is valid only when integrated over closed circuits, suggesting that a different form, known as the Neumann form, can yield balanced forces.
  • A participant introduces the idea that electromagnetic fields carry momentum, which complicates the application of Newton's laws in electrodynamics, although pseudo-mechanical formulations exist.
  • Some participants assert that Newton's third law does apply for constant currents in closed loops, with one clarifying that they did not mean to imply it is never valid in electromagnetism.
  • Another participant expresses interest in discussing the microscopic modeling of forces in a wire and questions whether MHD could provide clearer insights into the ambiguities discussed.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of Newton's third law in electromagnetism, particularly in relation to current elements and closed circuits. There is no consensus on the implications of the Ampère force law or the role of electromagnetic fields in this context.

Contextual Notes

Limitations include the dependence on the definitions of current elements and the conditions under which the Ampère law is applied. The discussion also touches on unresolved aspects of modeling forces at a microscopic level.

Who May Find This Useful

This discussion may be of interest to those studying electromagnetism, particularly in relation to force laws, the implications of electromagnetic fields, and the intersection of classical mechanics and electrodynamics.

lalbatros
Messages
1,247
Reaction score
2
This is apparently a well known topic, but I did not know it before today.
Let us consider the Ampère law for the force experience by a current element (1) in the magnetic fields of another current elment (2):

[tex]\mathbf{dF}_{12} = \frac {\mu_0} {4 \pi} I_1 I_2 \frac {d \mathbf{s_2}\ \mathbf{ \times} \ (d \mathbf{s_1} \ \mathbf{ \times } \ \hat{\mathbf{r}}_{12} )} {r_{12}^2}[/tex]

You can easily check that the "action and reaction" are not balanced by the Ampère law since:

[tex]\mathbf{dF}_{12} + \mathbf{dF}_{21} <> 0[/tex]

How should we understand that?
 
Physics news on Phys.org
That force law is only valid if ds_1 and ds_2 are integrated over closed circuits.
Then a little vector calculus can be used to put it into a different form that does have
F_12=F_21. This form is called the Neumann form. It depends on the dot product of
ds_1 and ds_2.
This is shown in most EM textbooks.
 
It's a fascinating fact that the electromagnetic field itself carries momentum in classical electrodynamics, and this causes Newton's third law to appear to fail. For this reason it is intractable to use Newton's laws in electrodynamics (it is not impossible, there are pseudo-mechanical formulations of E&M, including Maxwell's own model, that allow us to apply Newtonian mechanics to find the missing reaction forces and momentum, but no one does this). Instead it is more convenient to use Lagrangian methods and/or the covariant formulation of E&M i.e. the faraday tensor, etc.
 
But NIII does apply for constant currents in closed loops.
 
clem said:
But NIII does apply for constant currents in closed loops.

Thanks for clarifying this point, I did not mean to imply that NIII is never valid in electromagnetism.
 
Thanks clem, I found the symmetric form in Jackson.
I realize of course that a current element can never exist outside of a closed circuit.
Therefore, in itself, the force on a current element alone could never be measured and could probably not be defined without ambiguity.
On the other hand microscopic forces can be clearly defined and verified experimentally.
Therefore, one can clearly say that current element are not really part of "fundamental physics".

However, I would be interrested by a extended discussion of this topic.
For example, would it not be possible to modelize the forces in a wire from a miscroscipic point of view?
Also, I will go back to my MHD notes and see if it could improve my understanding of this topic.
In MHD, would this ambiguity remain as such or would it be easier to understand?

Thanks
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K