2022/01/04 by Hubert Baty, Baty, Hubert
Physics and Astronomy · #Cosmology and Gravitation Theories #FOS: Physical sciences #High Energy Physics - Theory (hep-th) #Ionosphere and magnetosphere dynamics #Solar and Space Plasma Dynamics #Solar and Stellar Astrophysics (astro-ph.SR) #astro-ph.SR #hep-th
paper · pdf · doi:10.48550/arxiv.2201.01135
16 pages, 13 figures
arxiv created 2022/01/04 · openalex publication_date 2022/01/04 · arxiv updated 2022/01/05 · openalex created_date 2022/04/03 · openalex updated_date 2026/07/28
We revisit the well known Sweet-Parker (SP) model for magnetic reconnection in the framework of two dimensional incompressible magnetohydrodynamics. The steady-state solution is re-derived by considering a non zero viscosity via the magnetic Prandtl number Pm. Moreover, contrary to the original SP model, a particular attention is paid to the possibility that the inflowing magnetic field Be and the length of the current layer L are not necessarily fixed and may depend on the dissipation parameters. Using two different ideally unstable setups to form the current sheet, namely the tilt and coalescence modes, we numerically explore the scaling relations with resistivity η and Prandtl number Pm during the magnetic reconnection phase, and compare to the generalized steady-state SP theoretical solution. The usual Sweet-Parker relations are recovered in the limit of small Pm and η values, with in particular the normalized reconnection rate being simply S-1/2 (1 + Pm)-1/4, where S represents the Lundquist number S = LVA/η (VA being the characteristic Alfvén speed). In the opposite limit of higher Pm and/or η values, a significant deviation from the SP model is obtained with a complex dependence Be (η, Pm) that is explored depending on the setup considered. We discuss the importance of these results in order to correctly interpret the numerous exponentially increasing numerical studies published in the literature, with the aim of explaining eruptive phenomena observed in the solar corona.