Discrepancies with Maxwell's Eqns - vector potentials

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Discussion Overview

The discussion revolves around discrepancies in the representation of vector and scalar potentials in Maxwell's Equations, particularly focusing on Ampere's law. Participants explore different notations and conventions used in various texts and papers related to electromagnetic theory.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • VV5 identifies a discrepancy between the expression of Ampere's law in their textbook and a referenced paper, specifically regarding the signs and terms associated with the scalar and vector potentials.
  • DuckAmuck suggests that the differences in notation may be due to unit conversions and conventions commonly used in electromagnetic theory.
  • VV5 questions the physical implications of the ratio provided by DuckAmuck, seeking clarification on its meaning.
  • DuckAmuck responds that the differences are largely due to writing conventions and do not have significant physical implications, providing an analogy with conventions in particle physics.

Areas of Agreement / Disagreement

Participants express differing views on the implications of the notational differences, with some suggesting they are merely conventions while others seek deeper understanding of their physical significance. The discussion remains unresolved regarding the implications of these discrepancies.

Contextual Notes

Participants acknowledge that various conventions exist in electromagnetic theory, which may lead to confusion when comparing different sources. The discussion highlights the importance of understanding the context in which these equations are presented.

VictorVictor5
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Greetings all,

Trying to resolve a discrepancy with vector and scalar potentials with Maxwell's Equations, specifically Ampere's law.

In my E&M textbook (Balanis, 1989, Eqn 6-17), Ampere's law with a magnetic vector potential and electric scalar potential can be expressed as

[tex]E= -\nabla\phi-j \omega A[/tex]

where [tex]\phi[/tex] is the electric scalar potential, and A is the magnetic vector potential.

Now, in a paper I am referencing in my work, I see Ampere's expressed as the following:

[tex]E=-j \omega(A- \nabla \phi)[/tex]

When you distribute this equation, you get the [tex]-j \omega A + j \omega \nabla \phi[/tex]

where now the scalar potential is positive, and also has a [tex]j \omega[/tex] in front of it, where the first equation doesn't.

Is it because of the scalar potential being arbitrary since it's a function of position? Or is there something else?

I also checked Harrington, but no luck there either.

Thanks!
VV5
 
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My guess is the notation in the paper, compared to the notation you're used to is related by [tex]\phi = -\frac{\phi}{jw}[/tex]

So it's just a unit conversion basically. You see this a lot in EM. There's several different conventions.
 
DuckAmuck,

First, thanks for the reply.

Question for you. While the ratio you provided would work, and given that -j * -j = well, j^2, = -1 and the equation would work, but quick question. The ratio you provided - physically what would that mean?

Thanks again!
VV5
 
VictorVictor5 said:
DuckAmuck,

First, thanks for the reply.

Question for you. While the ratio you provided would work, and given that -j * -j = well, j^2, = -1 and the equation would work, but quick question. The ratio you provided - physically what would that mean?

Thanks again!
VV5

It's just a unit convention. For example, in particle physics we like to set speed of light equal to 1, for simplicity, so we're not writing "c" over and over. So E=mc^2 becomes E=m. The consequence of this is that energy and mass are in the same units, which is okay, just something to keep in mind when doing problems.

It doesn't really mean much *physically*, it's just a writing convention. And actually, the convention I'm used to doesn't even use j, all components are real. :)
 
Great - thanks so much for your help!

VV5
 
VictorVictor5 said:
Great - thanks so much for your help!

VV5

What I generally try to do is work through what the paper does in the convention I'm used to.
 

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