Abstract
Regarding new bipolar magnetic regions as sources of flux, we have simulated the evolution of the radial component of the solar photospheric magnetic field during 1976–1984 and derived the corresponding evolution of the line-of-sight polar fields as seen from Earth. The observed timing and strength of the polar-field reversal during cycle 21 can be accounted for by supergranular diffusion alone, for a diffusion coefficient of 800 km2 s-1. For an assumed 300 km2 s-1 rate of diffusion, on the other hand, a poleward meridional flow with a moderately broad profile and a peak speed of 10 m s-1 reached at about 5° latitude is required to obtain agreement between the simulated and observed fields. Such a flow accelerates the transport of following-polarity flux to the polar caps, but also inhibits the diffusion of leading-polarity flux across the equator. For flows faster than about 10 m s-1 the latter effect dominates, and the simulated polar fields reverse increasingly later and more weakly than the observed fields.
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Laboratory for Computational Physics and Fluid Dynamics.
E. O. Hulburt Center for Space Research.
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DeVore, C.R., Sheeley, N.R. Simulations of the sun's polar magnetic fields during sunspot cycle 21. Sol Phys 108, 47–59 (1987). https://doi.org/10.1007/BF00152076
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DOI: https://doi.org/10.1007/BF00152076