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      Sub-Grid-Scale Description of Turbulent Magnetic Reconnection in Magnetohydrodynamics

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          Abstract

          Magnetic reconnection requires, at least locally, a non-ideal plasma response. In collisionless space and astrophysical plasmas, turbulence could permit this instead of the too rare binary collisions. We investigated the influence of turbulence on the reconnection rate in the framework of a single fluid compressible MHD approach. The goal is to find out, whether unresolved, sub-grid for MHD simulations, turbulence can enhance the reconnection process in high Reynolds number astrophysical plasma. We solve, simultaneously with the grid-scale MHD equations, evolution equations for the sub-grid turbulent energy and cross helicity according to Yokoi's model (Yokoi (2013)) where turbulence is self-generated and -sustained through the inhomogeneities of the mean fields. Simulations of Harris and force free sheets confirm the results of Higashimori et al. (2013) and new results are obtained about the dependence on resistivity for large Reynolds number as well as guide field effects. The amount of energy transferred from large to the small scales is enhanced in case of fast turbulent reconnection and energy spectra are used to interpret the obtained regime of reconnection controlled by the turbulence timescale \(\tau_t\). The overall process is even faster for larger Reynolds numbers controlled by the background molecular resistivity \(\eta\), as long as the initial level of turbulence is not too large. This implies that turbulence plays an important role on fast reconnection at situation of large Reynolds number while the amplitude of turbulence can still be small.

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          Most cited references24

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          Sweet's mechanism for merging magnetic fields in conducting fluids

          E. Parker (1957)
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            The Solar Wind as a Turbulence Laboratory

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              Instability of current sheets and formation of plasmoid chains

              Current sheets formed in magnetic reconnection events are found to be unstable to high-wavenumber perturbations. The instability is very fast: its maximum growth rate scales as S^{1/4} v_A/L, where L is the length of the sheet, v_A the Alfven speed and S the Lundquist number. As a result, a chain of plasmoids (secondary islands) is formed, whose number scales as S^{3/8}.
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                Author and article information

                Journal
                2015-11-13
                2015-11-29
                Article
                10.1063/1.4947211
                1511.04347
                9562ed7a-b027-4584-8f7e-c7d3955d134c

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                11 pages, 17 figures, will be submitted to Physics of Plasmas (PoP)
                physics.plasm-ph physics.space-ph

                Plasma physics,Space Physics
                Plasma physics, Space Physics

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