  The Landau--Lifshitz equation describes the dynamics of magnetization inside
a ferromagnet. This equation is nonlinear and has an infinite number of stable
equilibria. It is desirable to control the system from one equilibrium to
another. A control that moves the system from an arbitrary initial state,
including an equilibrium point, to a specified equilibrium is presented. It is
proven that the second point is an asymptotically stable equilibrium of the
controlled system. The results are illustrated with some simulations.
