Duality transformation of the far field fields.
Duality transformation of the far field fields.
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We’ve seen that the far field electric and magnetic fields associated with a magnetic vector potential were
\begin{equation}\label{eqn:dualFarField:40} \BE = -j \omega \textrm{Proj}_\T \BA, \end{equation} \begin{equation}\label{eqn:dualFarField:60} \BH = \inv{\mu_0} \kcap \cross \BE. \end{equation}
It’s worth a quick note that the duality…
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