Numerical MHD Simulations of Reconnection in Solar Flares: Effects of the Magnetic-Field Strength in the Current Sheet

被引:0
|
作者
Izquierdo-Guzman, I. [1 ]
Gonzalez-Aviles, J. J. [2 ,3 ]
Guzman, F. S. [1 ]
机构
[1] Univ Michoacana, Inst Fis & Matemat, Edificio C-3, Morelia 58040, Michoacan, Mexico
[2] Univ Nacl Autonoma Mexico, Serv Clima Espacial Mexico, Lab Nacl Clima Espacial, Mexico CONAHCYT,Inst Geofis,Unidad Michoacan, Morelia 58190, Michoacan, Mexico
[3] Univ Nacl Autonoma Mexico, Escuela Nacl Estudios Super, Unidad Morelia, Morelia 58910, Michoacan, Mexico
关键词
Flares; dynamics; models; Magnetic fields; corona; Magnetic reconnection; theory; Magnetohydrodynamics; MAGNETOHYDRODYNAMIC SIMULATION; RESISTIVITY; MECHANISM; CODE; CAFE;
D O I
10.1007/s11207-023-02202-w
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We simulate the evolution of reconnection in solar flares to study the influence of magnetic-field strength and thermal conduction on the dynamics of the magnetic-reconnection and energy-conversion processes. For this, we solve the 2.5D resistive magnetohydrodynamics (MHD) equations with thermal conduction on a domain that contains the chromosphere-corona interface. The flare is triggered at a null point where a Gaussian resistivity distribution is maximum, and further evolution is tracked. The parameter space considers magnetic-field strength [B-0] between 22 G and 50 G, and thermal conductivity [kappa] in the range from zero to 10(-11) W m(-1)K(-7/2). In this parameter space, we find that the magnetic field determines the reconnection rate, which can change by a 100% in the range of B-0, whereas thermal conduction can induce a rate change of at most 10%. We also measure the evolution of magnetic, internal, and kinetic energies in a region just above the reconnection point and measure their interplay. For all simulations, magnetic energy dominates initially and relaxes on a time scale of about 20 seconds. In this interval, the magnetic energy drops by approximate to 50%, whereas the internal energy grows by approximate to 100%. During the process, part of the energy becomes kinetic, which pushes the reconnection jet upwards and is bigger for the bigger B-0 and smaller kappa.
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页数:20
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