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Fig. 3.
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Integration surface (pink) over which we evaluate Poynting’s theorem. It extends from r1 = rH up to r2 = 25rg < rpml and from θ = 0 to θ2 = 89° (just outside the equatorial disk). We decompose contributions to Poynting’s theorem into the terms shown. In the expressions, S ≡ cE × H/4π. We define
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