The back way for deriving Maxwell's Equations: from charge conservation?

In summary, the conversation discusses the derivation of Maxwell's equations from gauge symmetry and charge conservation. There is disagreement about the validity of certain publications and the role of gauge symmetry in deriving conservation laws. The thread is eventually closed due to high moderation and potential bias from one of the participants.
  • #1
timeant
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I found one article in 1993 talking about it.[Unacceptable reference deleted by the Mentors]
 
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  • #3
This is my favourite one:
https://iopscience.iop.org/article/10.1088/0143-0807/36/6/065036/pdf

There is a bit more that can be said about the derivation regarding where that e comes from but will leave it there at the moment. It becomes clearer when you see the derivation from Guage symmetry:
https://quantummechanics.ucsd.edu/ph130a/130_notes/node296.html

But it is well known the fundamental basis of EM is gauge symmetry. Noether's Theorem basically says symmetry leads to a conservation law and conversely. The conservation law from gauge symmetry is charge conservation, so it is hardly surprising that it also leads to Maxwell's equations. I have seen several 'derivations', and they all really boil down to gauge symmetry or charge conservation - plus relativity, of course.

Thanks
Bill
 
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  • #4
From a local gauge symmetry you don't get a uniquely defined conserved quantity, because gauge symmetry is rather a redundance in the description of a physical situation, i.e., the vector potential is not uniquely defined from the dynamical equations but only up to a gauge transformation, but vector potentials that differ only by a gauge transformation describe the same physical situation, i.e., the indeterminacy of the potentials is irrelevant for the description of the physical situation.

The electric charge (or the electric-charge four-current) conservation follows from the corresponding global symmetry and is a necessary condition for the consistency of the gauge theory. For details see

https://www.osti.gov/servlets/purl/6129984/ (preprint)
https://doi.org/10.1119/1.16219 (paper)
 
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  • #5
[UPDATE -- Quote Box with link to unacceptable reference deleted]

Are those spam links at the end of the PDF paper that you linked to? What are those? They look misplaced in a scientific publication...

[UPDATE -- Image of spam in the unacceptable reference deleted]
 
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  • #6
berkeman said:
Are those spam links at the end of the PDF paper that you linked to? What are those? They look misplaced in a scientific publication...

https://www.physicsforums.com/attachments/283358

Yes, it is an issue that needs to be sorted out. We do not promote 'spam' here.

Thanks
Bill
 
  • #7
EM gauge symmetry leads to conservervation laws having no physical meaning.
Electric charge conservation law can be derived from Dirac field's gauge symmetry by Noether theorem, not by EM field.
 
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  • #8
Nowdays one must be very careful, whether you really are looking at a scientific publication or not. That's a great example. Having spam in a "scientific paper" let's look it at least much more suspicious than other publications. The claim in the abstract that that's something new is for sure wrong. For sure already Maxwell was aware of the continuity equation for electric charge and current following from his laws.
 
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  • #9
timeant said:
EM gauge symmetry does not lead to conservervation laws having no physical meaning.
Charge conservation law can be derived from Dirac field's gauge symmetry by Noether theorem, not by EM field.
It can be derived from the global symmetry not from the local one. That's a subtle point and one should think it through carefully. See the AJP paper quoted in #4.
 
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  • #10
vanhees71 said:
It can be derived from the global symmetry not from the local one. That's a subtle point and one should think it through carefully. See the AJP paper quoted in #4.
Free EM fields are built up by ##A_{\mu}##. Electric charge density and current, which is irrelevant ##A_\mu##, are built by Dirac's ##\psi##.

I think you all should care about the academics, not the useless links.
 
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  • #11
timeant said:
I think you all should care about the academics, not the useless links.
Thread is closed for Moderation...
 
  • #12
Update -- After a Mentor discussion the unacceptable reference in the OP has been deleted and the thread is reopened.
 
  • #13
A few points:

(1) If it's a scientific paper, it doesn't have spam in it. Full stop.

(2) I don't believe you are here to ask questions. I believe you are here to push your own point of view. That's based on what you have written in this and other threads.

(3) That makes (1) even stronger. BTW, did you write it?

(4) To answer your original question, "The back way for deriving Maxwell's Equations: from charge conservation?", you can't. There are other theories with charge conservation that have different "Maxwell Equations" - Proca Electrodynamics and Calssical Yang-Miles to name but two.
 
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  • #14
The moderation rate in this thread is significantly higher than the posting rate. A sure sign to close it.

Thread closed.
 
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1. What is the "back way" for deriving Maxwell's Equations?

The "back way" for deriving Maxwell's Equations refers to the method of starting with the principle of charge conservation and using it to derive the four equations that describe the behavior of electric and magnetic fields.

2. Why is the "back way" considered an alternative method for deriving Maxwell's Equations?

The traditional method for deriving Maxwell's Equations begins with the four equations and uses them to show that charge conservation is a consequence. The "back way" reverses this process, starting with charge conservation and deriving the four equations.

3. How does the "back way" for deriving Maxwell's Equations relate to the principle of charge conservation?

The "back way" relies on the principle of charge conservation, which states that the total amount of electric charge in a closed system remains constant over time. By using this principle, the four equations that describe the behavior of electric and magnetic fields can be derived.

4. What are the advantages of using the "back way" for deriving Maxwell's Equations?

The "back way" allows for a deeper understanding of the fundamental principles behind Maxwell's Equations. It also provides an alternative perspective and can lead to new insights and discoveries in the field of electromagnetism.

5. Are there any limitations to using the "back way" for deriving Maxwell's Equations?

The "back way" may not be as straightforward as the traditional method for deriving Maxwell's Equations. It also requires a strong understanding of the principle of charge conservation and mathematical skills to manipulate equations. Additionally, it may not be suitable for all situations and may not always yield the same results as the traditional method.

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