In both electrostatic and magnetostatic finite element analysis the ne
ed occasionally arises for the inclusion of isolated perfect electric
and magnetic conductors, respectively. The surfaces of such conductors
represent equipotentials but do not constitute a Dirichlet boundary c
ondition. Existing methods for constraining such surface potentials to
be constant, without giving specific values, are fairly complicated.
This paper presents a simple approach which requires no modifications
to existing finite element programs that can solve Laplace's and Poiss
on's equation subject to the usual Dirichlet and Neumann boundary cond
itions. The paper also addresses the dual problem of voids in conducto
rs and shows how the floating potential concept can be exploited to ob
tain streamlines of current flow.