1970 Volume 24 Issue 6 Pages 313-318
As it was pointed out by A.Simon, a set of equations governing the well-known magneto-static equilibrium do not yield an unique solution. The problem may be solved by making use of the following London equation, j=e2 (1/me+1/mi) nA,
where j is the current density, me the mass of electron, mi the mass of ion, n the number density of electron and A the vector potential.