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.