Abstract
We consider an isothermal ferrofluid layer which is nearly inviscid and semi-infinite. It is subjected to a magnetic field that consists of two parts. The first one is a vertical constant component. The second part is oscillating with time in a vertical plane. The linearized Laplace law describing the deformation of the free surface reduces to the study of a Hill equation, thus generalizing the Mathieu equation studied for a purely oscillating magnetic field. Using a classical method, we derive the marginal oscillating conditions and compare them with experimental situations.
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Hennenberg, M., Slavtchev, S. & Valchev, G. On the Hill Equation Describing Oscillations of a Ferrofluid Free Surface in a Vertical Magnetic Field. Microgravity Sci. Technol. 22, 455–460 (2010). https://doi.org/10.1007/s12217-010-9221-x
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DOI: https://doi.org/10.1007/s12217-010-9221-x