Lienard Wiechert potential of a point charge ?

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SUMMARY

The discussion centers on the Lienard-Wiechert (LW) potential of a point charge, specifically addressing the validity of the equation \(\frac{e}{r}|_{t-r/c}\) as a solution to the retarded potential integral. Participants highlight that this equation is incorrect because it cannot be derived from fundamental equations and does not represent the total charge density. The conversation references Heitler's "Quantum Theory of Radiation" and suggests that a deeper understanding of the mathematical derivation is necessary, particularly regarding the implications of special relativity and the behavior of charge distributions.

PREREQUISITES
  • Understanding of Lienard-Wiechert potentials
  • Familiarity with retarded potentials in electromagnetism
  • Knowledge of special relativity principles
  • Basic calculus, particularly differentiation and integration techniques
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  • Study the derivation of Lienard-Wiechert potentials in detail
  • Learn about the implications of special relativity on electromagnetic theory
  • Explore the mathematical techniques for calculating charge density distributions
  • Review section 2.10 of relevant texts for retarded time differentiation methods
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This discussion is beneficial for physicists, particularly those specializing in electromagnetism and quantum field theory, as well as students seeking to deepen their understanding of charge dynamics and potential theory.

snapback
Good day to everybody,

I got stuck at certain (basic) question regarding Lienard Wiechert (LW) potential of a point charge:

In Heitler's great book "Quantum Theory of Radiation" (I've used the edition from 1954), on page 18, there is a familiar statement that:
\frac{e}{r}|_{t-r/c} is not a valid solution of the retarded potential integral. Heitler justification why this result is wrong is somewhat unclear to me: he states that if "the integral \int \rho(P',t')dr' would not represent the total charge". Does anybody has any idea how the explicit mathematical calculation works in this case or where it could be found ?

I consulted few books (e.g. Jackson, Feynman II, Chapter 20) but only found a derivation of LW potentials (but Feynman nevertheless states, that the above given simple equation is worng, but he also does not give any mathematical justification"

thank you for your kind help
 
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The e/r equation is wrong because it cannot be derived from more basic equations, and it does not equal the L-W potential which is derived.
 
snapback said:
In Heitler's great book "Quantum Theory of Radiation" (I've used the edition from 1954), on page 18, there is a familiar statement that:
\frac{e}{r}|_{t-r/c} is not a valid solution of the retarded potential integral. Heitler justification why this result is wrong is somewhat unclear to me: he states that if "the integral \int \rho(P',t')dr' would not represent the total charge". Does anybody has any idea how the explicit mathematical calculation works in this case or where it could be found ?

There is an additional effect, similar to a shockwave. The potential is "compressed"
in front of the moving charge and stretched behind it. It's all explained in detail in
chapter 2 of my book.


http://www.physics-quest.org/Book_Chapter_EM_LorentzContr.pdf


Regards, Hans
 
glad to see your answers !

I would rather consider the e/r equation as "guessed", but guessing does not automatically means an answer being wrong, since, for example, you can solve integrals by "guessing" (even it is not the usual way of calculating stuff). But when you guess a solution, you of course need to verify, that it is really a solution by doing the calculation "backwards" (e.g. by differentiating the integral).

Coming back to my previous question: do you know where such"backward" calculation which clearly shows that the e/r-solution does not yield the correct charge density can be found ?

Thanks
 
snapback said:
glad to see your answers !

I would rather consider the e/r equation as "guessed",

Why consider the wrong answer?? It violates special relativity.
There would be no Lorentz contraction if true.

snapback said:
but guessing does not automatically means an answer being wrong, since, for example, you can solve integrals by "guessing" (even it is not the usual way of calculating stuff). But when you guess a solution, you of course need to verify, that it is really a solution by doing the calculation "backwards" (e.g. by differentiating the integral).

Coming back to my previous question: do you know where such"backward" calculation which clearly shows that the e/r-solution does not yield the correct charge density can be found ?

Thanks
That would be a (very) complicated and not straightforward calculation. If you perfectly
understand all the calculations done in the Lienard-Wiechert theory then you might start
to think about doing things like this.

The answer would be a moving point charge density distribution which, when at rest, would
have a non spherical potential field: An ellipsoid.

A point charge which would do this contains an infinite series of higher order dipole moments,
described by an infinite series of higher order differentials of Dirac impulse functions.

You don't get something like that rolling out straightforwardly from taking the d'Alembertian.
Taking derivatives from a retarded potential is trickier then taking the derivatives from a
normal function. Try to understand section 2.10 where the electrical field is derived from
the potential field.

http://www.physics-quest.org/Book_Chapter_EM_LorentzContr.pdfRegards, Hans
 
Hans de Vries said:
Why consider the wrong answer?? It violates special relativity.
There would be no Lorentz contraction if true.

First of all I would like to cite N. Bohr in a fairly sloppy manner:
When it comes to atoms, language can be used only as in poetry.

what I'm searching for is not some sentences in words, that everybody might understand in a different way, NO!, I precisely want to see that thing which you described as

Hans de Vries said:
an infinite series of higher order dipole moments,
described by an infinite series of higher order differentials of Dirac impulse functions.
,

so that the
Hans de Vries said:
would
will turn into is.

I simply want to see the technique applied, regardless whether the solution is right or wrong and wright. So I would equally be glad to see that the "proper" solutions namely eqn. (2.4) and (2.5) in your chapter 2 really lead to the proper charge and current density (kind of generalized procedure of taking d'Alembertian)

Anyway, I will try to follow the hints in section 2.10 with the "retarded time differentiation" + chain rule, this looks interesting.

have a nice saturday
 

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