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Instability of a planar liquid layer in an alternating magnetic field

Published online by Cambridge University Press:  20 April 2006

E. J. McHale  and
J. R. Melcher
E. J. McHale
Affiliation:
Massachusetts Institute of Technology, Department of Electrical Engineering and Computer Science, Cambridge, Mass. 02139 U.S.A.
J. R. Melcher
Affiliation:
Massachusetts Institute of Technology, Department of Electrical Engineering and Computer Science, Cambridge, Mass. 02139 U.S.A.
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Abstract

Liquid metal interfaces, stressed by a high-frequency, alternating magnetic field are commonly observed to undulate. Even a planar interface stressed from above by a uniform magnetic field takes on an appearance that is very different from what is observed if the same layer is heated from below with about the same thermal input as associated with the eddy currents. This behaviour affects internal mixing and the transport of heat and material from interfaces. In applications where the interface is used to form glass or other materials, the undulations can be disasterous. A goal of this paper is to identify the circumstances under which this motion can be avoided. A theoretical model is developed for fluid motions, coupled to a magnetic flux density (having magnitude B0 and angular frequency ω) through a force density that is time averaged over one period of the alternating field. This theory, which does not include thermal effects, predicts a threshold for onset of instability determined by the ratio of layer thickness to skin depth and by the parameter M = B02/μηω where μ = 4π × 10−7 and and η is the viscosity. The instability has an internal nature in that it is predicted even when the liquid is bounded by rigid insulating materials. Threshold measurements are reported that agree with the predictions over more than an order-of-magnitude variation in frequency, including low frequencies, for which the finite depth of the liquid layer is important. However, observed growth times are far shorter than predicted. It is concluded that the observed motions are in fact thermally driven, but take on an appearance dictated by the hydromagnetics. A previously developed lumped parameter model, which includes thermally driven motion, does predict growth times on the order of those observed. In the lumped parameter model the critical field strength grossly affects the nonlinear saturation velocity. The critical M sets an upper limit on the extent to which a liquid metal can be levitated, depressed or transported magnetically at a given frequency without incurring interfacial undulations and an augmentation of mass and heat transfer.

Type
Research Article
Information
Journal of Fluid Mechanics , Volume 114 , January 1982 , pp. 27 - 40
Copyright
© 1972 Cambridge University Press

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References

Betchov, R. & Criminale, O. 1967 Stability of Parallel Flows, chap. 3. Academic.
Chandrasekhar, S. 1961 Hydrodynamic and Hydromagnetic Stability. Clarendon.
Fraser, M. E., Lu, W. K., Hamiclec, A. E. & Murarka, R. 1971 Surface tension measurements on pure liquid iron and nickle by an oscillating drop technique. Metallurgical Trans. 2, 817.Google Scholar
Hoffman, K. & Kunze, R. 1961 Linear Algebra. Prentice-Hall.
Mchale, E. J. 1977 AC magnetohhydrodynamic instability, Ph.D. thesis, Department of Electrical Engineering, Massachusetts Institute of Technology.
Mchale, E. J. & Melcher, J. R. 1978 Hydromagnetic instability of liquid metals in AC magnetic fields, and augmentation of heat transfer. Electric Machines & Electromech. 3, 197.Google Scholar
Melcher, J. R. 1981 Continuum Electromechanics, pp. 6.20–6.22 and 8.1–8.15. MIT Press.
Melcher, J. R. & Hurwitz, M. 1970 U.S. Patent 3,496,736.
Schaffer, M. 1966 Hydromagnetic Surface Waves with an Alternating Magnetic Field. Ph.D. thesis, Department of Electrical Engineering, Massachusetts Institute of Technology.
Schaffer, M. 1968 Hydromagnetic surface waves with alternating magnetic fields. J. Fluid Mech. 4, 337.Google Scholar
Sunderlam, T. 1973 Thermal diffusion in kinetic and equilibrium measurements by a levitation technique. Metallurgical Trans. 4, 575.Google Scholar