Evolution of Three-dimensional Coherent Structures in Hall Magnetohydrodynamics
被引:7
|
作者:
Bora, K.
论文数: 0引用数: 0
h-index: 0
机构:
Udaipur Solar Observ, Phys Res Lab, Bari Rd, Udaipur 313001, Rajasthan, India
Indian Inst Technol, Discipline Phys, Gandhinagar 382355, IndiaUdaipur Solar Observ, Phys Res Lab, Bari Rd, Udaipur 313001, Rajasthan, India
Bora, K.
[1
,2
]
Bhattacharyya, R.
论文数: 0引用数: 0
h-index: 0
机构:
Udaipur Solar Observ, Phys Res Lab, Bari Rd, Udaipur 313001, Rajasthan, IndiaUdaipur Solar Observ, Phys Res Lab, Bari Rd, Udaipur 313001, Rajasthan, India
Bhattacharyya, R.
[1
]
Smolarkiewicz, P. K.
论文数: 0引用数: 0
h-index: 0
机构:
Natl Ctr Atmospher Res, POB 3000, Boulder, CO 80307 USAUdaipur Solar Observ, Phys Res Lab, Bari Rd, Udaipur 313001, Rajasthan, India
Smolarkiewicz, P. K.
[3
]
机构:
[1] Udaipur Solar Observ, Phys Res Lab, Bari Rd, Udaipur 313001, Rajasthan, India
[2] Indian Inst Technol, Discipline Phys, Gandhinagar 382355, India
[3] Natl Ctr Atmospher Res, POB 3000, Boulder, CO 80307 USA
Solar magnetic reconnection;
Magnetohydrodynamical simulations;
MAGNETIC RECONNECTION;
D O I:
10.3847/1538-4357/abc8f7
中图分类号:
P1 [天文学];
学科分类号:
0704 ;
摘要:
This work extends the computational model EULAG-MHD to include Hall magnetohydrodynamics (HMHD)-important to explore physical systems undergoing fast magnetic reconnection at the order of the ion inertial length scale. Examples include solar transients along with reconnections in magnetosphere, magnetotail, and laboratory plasmas. The paper documents the results of two distinct sets of implicit large-eddy simulations in the presence and absence of the Hall forcing term, initiated with an unidirectional sinusoidal magnetic field. The HMHD simulation while benchmarking the code also emphasizes the complexity of three-dimensional (3D) evolution over its two-dimensional counterpart. The magnetic reconnections onset significantly earlier in HMHD. Importantly, the magnetic field generated by the Hall term breaks any inherent symmetry, ultimately making the evolution 3D. The resulting 3D reconnections develop magnetic flux ropes (MFRs) and magnetic flux tubes. Projected on the reconnection plane, the ropes and tubes appear as magnetic islands, which later break into secondary islands, and finally coalesce to generate an X-type neutral point. These findings are in agreement with the theory and contemporary simulations of HMHD, and thus verify our extension of the EULAG-MHD model. The second set explores the influence of the Hall forcing on generation and ascend of an MFR from sheared magnetic arcades-a novel scenario instructive in understanding the coronal transients. The rope evolves through intermediate complex structures, ultimately breaking locally because of reconnections. Interestingly, the breakage occurs earlier in the presence of the Hall term, signifying faster dynamics leading to magnetic topology favorable for reconnections.