The Navier-Stokes equations and magnetohydrodynamics equations are written in terms of poloidal and toroidal potentials in a finite cylinder. This formulation insures that the velocity and magnetic fields are divergence-free by construction, but leads to systems of partial differential equations of higher order, whose boundary conditions are coupled. The influence matrix technique is used to transform these systems into decoupled parabolic and elliptic problems. The magnetic field in the induction equation is matched to that in an exterior vacuum by means of the Dirichlet-to-Neumann mapping, thus eliminating the need to discretize the exterior. The influence matrix is scaled in order to attain an acceptable condition number.
Motivation and Governing EquationsThe requirement that velocity and magnetic fields be solenoidal, i.e. divergence-free, represents one of the most challenging difficulties in hydrodynamics and in magnetohydrodynamics [1,2,3,4,5,6,7]. For the velocity field, this condition is the fundamental approximation used in incompressible fluid dynamics. For the magnetic field, this condition is the statement of the non-existence of magnetic monopoles.Two main approaches exist for imposing this requirement. The first is to use three field components and to project three-dimensional fields onto a divergence-free field. In an incompressible fluid, the pressure serves to counterbalance the nonlinear term which is the source of the divergence in the Navier-Stokes equations; the pressure also plays this role numerically. The divergence of the Navier-Stokes equations is taken, leading to a Poisson problem for the pressure. However, the boundary conditions on the