Now for McAdoo's Tenex, we will go the same route as we went for electrostatic, so we will start by
considering the Maxwell's equations.
So here you can see them again in general, but we want to consider Magneto Static's.
So we will use here only the actual equations that are concerned with the magnetic fields and we will
set all the time derivatives.
So for example, here, just partial derivative of E with respect to T to zero.
So this means we consider here to equation in this differential formulation and two equations in this
integral formulation.
So this is somewhat similar to electrostatic.
However, the main difference if we compare these equations here to the equations of electrostatic is
that now we have no divergences in the magnetic field while we had divergences in the electric field.
But we have instead rotations in the magnetic field while the rotations in the electric field where
zero for electrostatic.
So this means our equations are in some way similar, but also kind of different.
And we will now continue and investigate what this means for the solution of these equations.