The potential electric and vector potential of a moving charge

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The discussion focuses on the application of the Liénard-Wiechert equations to determine the electric and vector potentials of a moving charge. The participant presents a condition involving the particle's position and velocity, expressed mathematically, to establish the relationship between the electric potential and the distance from the charge. They also mention the vector potential derived from the current density and question whether their understanding aligns with established theories, particularly regarding the speed of potential propagation. There is a reference to Feynman's Lectures, emphasizing the nuances of gauge choices in electromagnetic theory. The inquiry seeks validation of their approach and understanding of these concepts.
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Relevant Equations
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I could try to apply the Liénard-WIechert equations immediatally, but i am not sure if i understand it appropriately, so i tried to find by myself, and would like to know if you agree with me.

When the information arrives in ##P##, the particle will be at ##r##, such that this condition need to be satisfied:
$$\frac{(vt-r)^2}{v^2} = \frac{r^2+b^2}{c^2} (1)$$

So, we have $$\phi = \frac{kq}{s} = \frac{kq}{r}$$
Also, $$ \vec A = \frac{\mu}{4\pi} \int \frac{J' dV'}{|r-r'|} = \frac{\mu}{4\pi} \frac{q v}{|r|}$$

such that r satisfies ##(1)##.

Is it right? Do you agree with it? I am asking because i remember to read somewhere that the potential electric not necessarilly need to move at speed of light, but i think this is the case in Lorenz gauge. I haven't assumed any gauge here.
 
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