The velocity-gauge vector potential A_2 = c∫(Phi_c - Phi^(v))dt is shown to satisfy the wave equation by four independent analytic proofs.
From Lorenz to Coulomb and other explicit gauge transformations,
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Reply to "Comments on work of Yang and Nevels 'Direct, analytic solution for the electromagnetic vector potential in any gauge' (arXiv:2507.02104)" by Onoochin (arXiv:2507.08042)
The velocity-gauge vector potential A_2 = c∫(Phi_c - Phi^(v))dt is shown to satisfy the wave equation by four independent analytic proofs.