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*From*: John Denker <jsd@av8n.com>*Date*: Fri, 29 Mar 2013 10:46:24 -0700

The Liénard-Wiechert potentials are discussed in Feynman volume II section 21-5. If

you have not re-read that section recently, I recommend you do so, but first let me

offer a few words (and diagrams) that might clarify a couple of concepts.

Issue #1 has to do with "retarded potentials". That's simple enough for a

particle that is not moving, or not moving very much ... but if the particle

is moving there are different positions and therefore different amounts of

retardation and it gets kinda confusing.

Issue #2 has to do with the mysterious factor that Feynman sticks in, to obtain

equation 21.29 from the previous unnumbered equation. Feynman devotes a couple

of complicated figures and an entire page of text to explaining this factor, but

not everybody considers the explanation easy to follow.

We can resolve both of these issues in grand style with the help of a spacetime

diagram. In particular, the mysterious factor just comes from geometry. It is

the density of source-points near the light-cone.

This is discussed in more detail, with diagrams, at

http://www.av8n.com/physics/lienard-wiechert.htm

I'm not even sure this counts as a relativity problem, but it reinforces (again!)

the lesson that it really pays to draw the spacetime diagram.

**Follow-Ups**:**Re: [Phys-L] Visualizing the Liénard-Wiechert Potentials***From:*brian whatcott <betwys1@sbcglobal.net>

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