FIG. 8: Eigenfunctions of the radial and azimuthal velocity and magnetic field for type 2 Super-HMRI in the global case as a function of (r, z) at small Pm = 10−3, the narrow gap η̂ = 0.85 and conducting boundary conditions on the cylinders. The parameters (β,Ro,Ha,Re) are the same as those in Fig. 6(b) and the axial wavenumber is chosen to be kzm = 24, at which the growth rate for the given values of these parameters reaches a maximum (peak on the blue curve in that panel).
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