“…For eddy current formulations based on the magnetic scalar potential in K a , a set of representatives that span the first cohomology basis [1] of K a , denoted as H 1 (K a ), are required, see for example [2]- [4]. The recent attempts to efficiently solve eddy-current problems based on this formulation have allowed the computational topology [1] in general, and computational cohomology in particular, to made its way into commercial [5], [6] and research [7], [8] electromagnetic simulation software.…”