Abstract
We examine by means of a local analysis the effects of an azimuthal magnetic field B(r) on the stability of a rapidly-rotating fluid subject to a radial temperature gradient, taking the ratio κ/η of thermal to magnetic diffusivities to be small, as in the Earth's core. According to this theory, previous results for the case Br are typical of a certain range of magnetic field profiles, but if B decreases with r faster than r −½ we find instead that (i) the critical Rayleigh number increases sharply as the magnetic field strength increases beyond “magnetostrophic” values and (ii) the recently-discovered magnetic instabilities triggered by bottom-heavy density gradients do not occur. If B increases with r faster than r 3/2, on the other hand, the major change to the Br picture of events is that the system becomes unstable to comparatively fast magnetic instabilities as soon as the field passes magnetostrophic values.

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