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scostep 2010 (stp12) - Leibniz-Institut für Atmosphärenphysik an der ...

scostep 2010 (stp12) - Leibniz-Institut für Atmosphärenphysik an der ...

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STP12 Abstracts<br />

Berlin, 12 - 16 July <strong>2010</strong><br />

SCOSTEP Symposium <strong>2010</strong><br />

Data-driven Modeling of Solar Storm<br />

Kus<strong>an</strong>o K<strong>an</strong>ya 1 , Yamamoto Tetsuya T. 1 , Inoue Satoshi 2 , Shiota Daiko 3 , Nishida Keisuke 4 , Kataoka<br />

Ryuho 5<br />

1 Solar-Terrestrial Environment Laboratory, Nagoya University, 2 National <strong>Institut</strong>e of Information<br />

<strong>an</strong>d Communications Technology, 3 RIKEN, 4 Kwas<strong>an</strong> Observatory, Kyoto University, 5 Interactive<br />

Research Center of Science, Graduate School of Science <strong>an</strong>d Engineering, Tokyo <strong>Institut</strong>e of<br />

Technology<br />

Solar storm caused by solar flare <strong>an</strong>d/or coronal mass ejection (CME) is major source of<br />

heliospheric <strong>an</strong>d geo-magnetospheric disturb<strong>an</strong>ce. However, the onset mech<strong>an</strong>ism of that is<br />

not well un<strong>der</strong>stood yet. Aiming at revealing the initiation mech<strong>an</strong>ism of solar storm, we have<br />

recently developed a new data-driven simulation model based on the observation by Solar<br />

Optical Telescope (SOT) onboard Hinode solar physics satellite. Our model consists of the<br />

following three different magnetohydrodynamic (MHD) simulations for solar flare, CME, <strong>an</strong>d<br />

ICME, respectively. For the flare model, we first calculated the nonlinear force-free field<br />

(NLFFF) of active region NOAA 10930 using the vector magnetogram observed by<br />

Hinode/SOT as the boundary condition, <strong>an</strong>d carried out the three-dimensional MHD<br />

simulation by imposing photospheric variation which corresponds to the magnetic flux<br />

emerging activity seen in the active region prior to the flare occurred on December 13, 2006.<br />

As a result, we have successfully simulated a solar eruption, in which magnetic reconnection<br />

drives super Alfvenic plasma jet from the flaring site. It was also shown that magnetic<br />

reconnection may initiate the tr<strong>an</strong>sfer of magnetic helicity out of the active region into a large<br />

scale magnetic loop. Second, we h<strong>an</strong>ded over the result of the flare model into the global<br />

corona model, <strong>an</strong>d restarted the simulation for CME formation process. As a result, it was<br />

shown that the magnetic loop, which was subject to the magnetic helicity injection due to the<br />

flaring reconnection, could exp<strong>an</strong>d to a CME. Finally, we have performed the interpl<strong>an</strong>etary<br />

space simulation, in which the CME with magnetic helicity was set on the inner boundary.<br />

The model successfully tracked the propagation of ICME up to the orbit of earth, <strong>an</strong>d<br />

simulated the variation of magnetic field <strong>an</strong>d velocity consistent with the in-situ observation<br />

by ACE satellite. All the results indicate that the series of data-driven simulations is a<br />

powerful tool for un<strong>der</strong>st<strong>an</strong>ding the entire process of solar storm. It also suggests that the<br />

process from flare to ICME should not be explained as a result of simple plasmoid ejection<br />

but is constituted of several stages, which might be governed by different processes of<br />

resistive <strong>an</strong>d ideal MHD.

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