We investigate the stability of interfacial waves in conducting fluids
under the influence of a vertical current density, paying particular
attention to aluminium reduction cells in which such instabilities are
commonly observed. We develop a wave equation for the interface in wh
ich the Lorentz force is expressed explicitly in terms of the fluid mo
tion. Our wave equation differs from previous models, most notably tha
t developed by Urata (1985), in that earlier formulations rested on a
more complex, implicit coupling between the fluid motion and the Loren
tz force. Our formulation furnishes a number of quite general stabilit
y results without the need to resort to Fourier analysis. (The need fo
r Fourier analysis typifies previous studies.) Moreover, our equation
supports both travelling and standing waves. We investigate each in tu
rn. We obtain three new results. First, we show that travelling waves
may become unstable in the presence of a uniform, vertical magnetic fi
eld. (Our travelling waves are quite different to those discovered by
previous investigators (Sneyd 1985 and Moreau & Ziegler 1986) which re
quire more complex magnetic fields to become unstable.) Second, in lin
e with previous studies we confirm that standing waves may also become
unstable. In this context we derive a simple energy criterion which s
hows which types of motion may extract energy from the background magn
etic held. This indicates that a rotating, tilted interface is particu
larly prone to instability, and indeed such a motion is often seen in
practice. Finally, we use Gershgorin's theorem to produce a sufficient
condition for the stability of standing waves in a finite domain. Thi
s allows us to place a lower bound on the critical value of the backgr
ound magnetic field at which an instability first appears, without sol
ving the governing equations of motion.