Question: Show that for any electromagnetic potentials (ɸ,A) there are many possible choices of gauge-transformed potentials such that the Lorentz condition (D.11) is satisfied. af =+

Show that for any electromagnetic potentials (ɸ,A) there are many possible choices of gauge-transformed potentials

af φ=φ+ Ət A = Á – Vf,

such that the Lorentz condition (D.11) is satisfied.

дФ + V·A = 0. дt (D.11)

af =+ t A = Vf, + VA = 0. t (D.11)

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