The model as stated is actually a two fluid problem with a positively charged fluid of ions and a negatively charged fluid of electrons. The mass of an electron is very small compared to the mass of an ion, thus we can represent the system as a single fluid that reacts with magnetic fields.
For this section we will assume that the plasma is incompressible. This approximation greatly reduces the complexity of the system of equations for the model. Using a simplified model that is easily verified provides a good benchmark for the more complex compressible model that we investigate in chapter 8.
The MHD equations have been treated numerically by many including
[61] and [62,63] using finite
differences and [64] using Fourier collocation. There
has been some disagreement about how to deal with the constraint that
no magnetic monopoles can exist (i.e. that
where B is the magnetic field). However, it has been shown in
[65] that the smallest errors in satisfying this
constraint can cause a significant cumulative effect as a simulation
progresses. We will test a magnetic streamfunction formulation for
the incompressible equations as this provides a formulation that fits
naturally into the set of operators that we developed in previous
chapters. A simple modification was needed to make the incompressible
Navier-Stokes code handle the extra field and interactions.