Abstract
This paper considers the stability of a horizontal liquid-metal
free surface in the
presence of a horizontal alternating magnetic field. A weak formulation
is used to
derive a generalized Mathieu–Hill equation for the evolution of surface
perturbations.
Previous studies which rely on time-averaging the electromagnetic force
over one field
cycle have predicted a generally weak instability, but we find much larger
growth rates
near the resonances, where the surface wave frequency is an integral multiple
of the
field frequency. The method can be extended to include viscous and ohmic
damping;
the former has little effect, while the latter damps all waves except those
whose
frequency is close to the field frequency. Growth rates can be closely
approximated
by simple algebraic formulae, as can the critical magnetic field strength
for the onset
of instability.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
23 articles.
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