Abstract
We consider the Poynting vector of two exact solutions describing a charged magnetized non-rotating mass in the following limiting cases: (i) m2 = q2, and (ii) m = 0. Whereas the former limit leads to a non–vanishing Poynting vector only for one of the solutions, the latter limit in both solutions results in non–zero expressions of the azimuthal component of the Poynting vector, thus providing evidence that Bonnor's frame–dragging effect takes place even in the case of a charged massless magnetic dipole.
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