Abstract: | By a general argument, it is shown that Maxwell–Herglotz‐fields are dense (with respect to the C∞(Ω)‐topology) in the space of all solutions to Maxwell's equations in Ω. This is used to provide corresponding approximation results in global spaces (e.g. in L2‐Sobolev‐spaces Hm(Ω)) and for boundary data. Proofs are given within the framework of generalized Maxwell's equations using differential forms. Copyright © 2004 John Wiley & Sons, Ltd. |