日本地球惑星科学連合2021年大会

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[E] 口頭発表

セッション記号 P (宇宙惑星科学) » P-EM 太陽地球系科学・宇宙電磁気学・宇宙環境

[P-EM09] Dynamics of Magnetosphere and Ionosphere

2021年6月6日(日) 09:00 〜 10:30 Ch.05 (Zoom会場05)

コンビーナ:藤本 晶子(九州工業大学)、尾崎 光紀(金沢大学理工研究域電子情報学系)、佐藤 由佳(日本工業大学)、中溝 葵(情報通信研究機構 電磁波研究所)、座長:長谷川 洋(宇宙航空研究開発機構宇宙科学研究所)、西野 真木(宇宙航空研究開発機構宇宙科学研究所)

09:05 〜 09:20

[PEM09-02] Magnetic Reconnection in a Sheared Magnetic Flux Tube: Slippage versus Tearing

*国吉 秀鷹1、Hesse Michael2、Nogren Cecilia3、Tenfjord Paul3、Kwagala Norah3 (1.東京大学地球惑星科学専攻、2.アメリカ航空宇宙局エイムズ研究センター、3.ベルゲン大学宇宙プラズマ物理学グループ)


キーワード:磁気リコネクション、オーロラ加速、電磁流体力学

Although it still remains controversial whether auroral acceleration is, in fact, a manifestation of a reconnection process, discussions of a different type of reconnection in this context began with 'reconnection type II' by Haerendel (Haerendel, 2007, 2011), which recognized early on that auroral acceleration may be a form of magnetic reconnection. According to the author, the reconnection process enhances the auroral acceleration by reducing the flux tubes’ shear magnetic stress of field aligned current sheets. The process of magnetic reconnection in a flux tube can occur in a time-stationary fashion as slippage reconnection or in a time-dependent manner, for example, tearing instability. However, it is not well known how a system can be set up to sustain slippage reconnection, whether there is a combination of slippage reconnection and time-dependent reconnection. To investigate this question, using a 3D MHD simulation, we model a twisted flux tube, adding a spatially localized resistive region in the center of the simulation box. As a result, firstly, the Poynting flux injected at the boundary propagates to the resistive region and dissipates there. Secondly, tearing instability occurs with slippage reconnection in the resistive region when the resistivity is strong enough and the cross section of the flux tube is elliptical enough, otherwise only slippage reconnection occurs. Finally, magnetic field generated by tearing instability propagates to both ends of the flux tube.