Magnetohydrodynamics evolution of three-dimensional magnetic null in NOAA active region 11515 initiated using non-force-free field extrapolation
arXiv:2210.03957 · doi:10.3389/fspas.2022.1039061
Abstract
Magnetohydrodynamics simulation of active region NOAA 11515 is performed to examine the initiation of the M5.6 flaring event that starts around 10:43 UT on 2012 July 2. The simulation is conducted using an extrapolated non-force-free magnetic field generated from the photospheric vector magnetogram of the active region as the initial magnetic field. The magnetic field shows the presence of a three-dimensional (3D) magnetic null with the corresponding dome overlying a filament and a low-lying magnetic flux rope, observed in 304~Å~ and 131~Å~ respectively. The simulated dynamics, triggered by the initial Lorentz force, lead to the bifurcations of the flux rope, which is similar to the observed bifurcation in the 131 Å~ brightenings. Additionally, the rope exhibits a rise and reconnects at the 3D null. These reconnections convert field lines of the rope into the anchored outer spine of the 3D null -- explaining the occurrence of a nearby confined C-class flare. Further, the results show that the field lines of the flux rope reach the vicinity of the filament and become non-parallel to the field lines of the filament. This initiates the reconnections between the rope and the field lines of the filament -- activating the filament for the eruption. This interesting interaction of the flux rope and filament seems to contribute to the onset of the M-class flare.
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References in corpus (22)
- The Helioseismic and Magnetic Imager (HMI) Vector Magnetic Field Pipeline: SHARPs -- Space-weather HMI Active Region Patches
- Structure, Stability, and Evolution of Magnetic Flux Ropes from the Perspective of Magnetic Twist
- Circular Ribbon Flares and Homologous Jets
- Nonlinear force-free modeling of the solar coronal magnetic field
- MHD Simulation of a Sigmoid Eruption of Active Region 11283
- Magnetohydrodynamic Modeling of the Solar Eruption on 2010 April 8
- The Magnetic Topology of Coronal Mass Ejection sources
- On the nature of reconnection at a solar coronal null point above a separatrix dome
- Magnetohydrodynamic Simulation of the X2.2 Solar Flare on 2011 February 15: I. Comparison with the Observations
- Magnetohydrodynamic Simulation of the X2.2 Solar Flare on 2011 February 15: II. Dynamics Connecting the Solar Flare and the Coronal Mass Ejection
- A Practical Approach to Coronal Magnetic Field Extrapolation Based on the Principle of Minimum Dissipation Rate
- Magnetohydrodynamic Simulation of Magnetic Null-point Reconnections and Coronal dimmings during the X2.1 flare in NOAA AR 11283
- Magnetohydrodynamic simulation of magnetic null-point reconnections in NOAA AR12192 initiated with an extrapolated non-force-free-field
- Why are flare ribbons associated with the spines of magnetic null points generically elongated?
- On the role of repetitive magnetic reconnections in evolution of magnetic flux-ropes in solar corona
- Magnetic reconnection at 3D null points: effect of magnetic field asymmetry
- Onset of a Large Ejective Solar Eruption from a Typical Coronal-Jet-Base Field Configuration
- An Eruptive Circular-ribbon Flare with Extended Remote Brightenings
- Sunspot splitting triggering an eruptive flare
- Comparison of Two Coronal Magnetic Field Models for Reconstructing a Sigmoidal Solar Active Region With Coronal Loops
- Lorentz Force Evolution Reveals the Energy Buildup Processes during Recurrent Eruptive Solar Flares
- Comparison of the Hall Magnetohydrodynamics and Magnetohydrodynamics evolution of a flaring solar active region
Cited by in corpus (3)
- Formation of an observed eruptive flux rope above the torus instability threshold through tether-cutting magnetic reconnection
- Magnetohydrodynamics simulation of magnetic flux rope formation in a quadrupolar magnetic field configuration
- Formation and rising phase of a flux rope through data-constrained simulations