2011/06/26 by Toby S. Wood, T. S. Wood, J. O. McCaslin +3
Physics and Astronomy · #Astrophysics and Star Formation Studies #Convection #Convection zone #Helioseismology #Magnetic field #Magnetohydrodynamics #Meridional flow #Rotation (mathematics) #Solar and Space Plasma Dynamics #Solar rotation #Stellar, planetary, and galactic studies #Tachocline #astro-ph.SR
paper · pdf · doi:10.1088/0004-637x/738/1/47
49 pages, 11 figures, in press in the Astrophysical Journal
arxiv created 2011/06/26 · openalex publication_date 2011/08/11 · arxiv updated 2015/05/28 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
To date, no self-consistent numerical simulation of the solar interior has succeeded in reproducing the observed thinness of the solar tachocline and the persistence of uniform rotation beneath it. Although it is known that the uniform rotation can be explained by the presence of a global-scale confined magnetic field, numerical simulations have thus far failed to produce any solution where such a field remains confined against outward diffusion. We argue that the problem lies in the choice of parameters for which these numerical simulations have been performed. We construct a simple analytical magnetohydrodynamic model of the solar interior and identify several distinct parameter regimes. For realistic solar parameter values, our results are in broad agreement with the tachocline model of Gough & McIntyre. In this regime, meridional flows driven at the base of the convection zone are of sufficient amplitude to hold back the interior magnetic field against diffusion. For the parameter values used in existing numerical simulations, on the other hand, we find that meridional flows are significantly weaker and, we argue, unable to confine the interior field. We propose a method for selecting parameter values in future numerical models.