The adjoint problem in the presence of a deformed surface: the example of the Rosensweig instability on magnetic fluids

Physics – Condensed Matter – Soft Condensed Matter

Scientific paper

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11 pages, 1 figure

Scientific paper

10.1142/S0217979202010105

The Rosensweig instability is the phenomenon that above a certain threshold of a vertical magnetic field peaks appear on the free surface of a horizontal layer of magnetic fluid. In contrast to almost all classical hydrodynamical systems, the nonlinearities of the Rosensweig instability are entirely triggered by the properties of a deformed and a priori unknown surface. The resulting problems in defining an adjoint operator for such nonlinearities are illustrated. The implications concerning amplitude equations for pattern forming systems with a deformed surface are discussed.

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