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Merging of coronal and heliosph eric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Re s., 107, 2002. 2004 年 10 年 14 年 年年年年年 ( 年年 ) 西
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Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

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Page 1: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Merging of coronal and heliospheric numerical two-dimensional MHD models

D. Odstrcil, et al., J. Geophys. Res., 107, 2002.

2004 年 10 月 14 日 太陽雑誌会 ( 速報 ) 西田

Page 2: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Introduction

• Space weather research involves a chain of various phenomena occurring simultaneously on different spatial and temporal scales.

• An integrated modeling approach is necessary for space weather research.

• This paper presents a demonstration of merged coronal and heliospheric 2-D MHD models.

Page 3: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Numerical Models

• Coronal Model– 2-D axisymmetric resistive MHD equations– Semi-implicit finite difference scheme using st

aggered values

• Heliospheric Model– 2-D axisymmetric ideal MHD equations– Explicit finite difference total-variation-diminis

hing high-resolution Lax-Friendrichs (TVDLF) scheme using cell-centered values

Page 4: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

• Merged numerical grid

Fig. 1

• Coronal Model– 200x300 grid points– Nonuniform mesh for th

e streamer

• Heliospheric Model– 340x240 grid points

• The output from the coronal model is used as a boundary condition for the heliospheric solutions

Page 5: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. 2

Ambient State in the corona

Page 6: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. 3

Ambient State in the heliosphere

Page 7: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. 4. Blue: 70°, Red: 80°, Black: 90°

Page 8: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Transient Disturbances

• The streamer products strongly sheared field lines that are nearly aligned with the neutral line; it is just a convenient mechanism.

• The sharing phase lasts 5.2 days.

• We reduce the magnetic flux at the photosphere to create a flux rope.

• After ~18 hours the arcade erupts.

Page 9: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

http://sprg.ssl.berkeley.edu/cism/

Page 10: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. 5

Page 11: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. 6. Blue: 70°, Red: 80°, Black: 90°

Page 12: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. 7

Page 13: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. 8

Page 14: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. 9

Page 15: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. 10 . Blue: 70°, Red: 80°, Black: 90°

Page 16: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Conclusions (1/2)

• The merging of coronal and heliospheric MHD models has been successfully implemented for a 2-D ambient state and a transient disturbance.

• Different mathematical models, numerical methods, and computational grids were used in this work, and thus the merging of the numerical models was demonstrated for a quote general case.

Page 17: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Conclusions (2/2)

• Merged coronal and heliospheric models have enabled the simulation of transient disturbances.

• The solar wind and magnetic parameters at 1 AU resulting from the coupled computations can provide input for geo-effectivity models.

Page 18: Merging of coronal and heliospheric numerical two-dimensional MHD models D. Odstrcil, et al., J. Geophys. Res., 107, 2002. 2004 年 10 月 14 日 太陽雑誌会 ( 速報.

Fig. A1