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RETARDED POTENTIALS I. In Statics We have seen that the potentials in statics are as follows: E = - ∇ φ, (I.1) with: Φ = (1/4πε0) ∫ ρ(r')d3r'/|r -r'| (I.2) B = ∇ x A (I.3) Coulomb gauge: ∇ . A = 0 (I.4) A(r) = μ0/4π∫ J(r') /|r-r'| d3(r') (I.5) II. In Dynamics II.1 ...
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Particular cases of a moving charge I. First case: Constant velocity. V and r are perpendicular In the following figure: the origin of the time is set when after the retarded time t'. We will express E and B at the time t. Th epoint od observation P is set a plane ...
