sources, namely, nonradiating (NR) sources and sources that lack a NR part, ie,“purely
radiating” sources. The class of purely radiating sources is shown to be exactly the class of
solutions—within the source's support—of the homogeneous form of the associated partial
differential equation relating the sources to their fields; ie, purely radiating sources are
themselves fields. We show that this result is related to the well-known reciprocity principle …