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Ensemble Modeling of Successive Halo CMEs: A Case Study
- 作者:C. O. Lee ; C. N. Arge ; D. Odstrcil ; G. Millward ; V. Pizzo ; N. Lugaz
- 关键词:Ensemble modeling ; Coronal mass ejections ; modeling ; Solar wind ; modeling ; Solar wind ; observations
- 刊名:Solar Physics
- 出版年:2015
- 出版时间:April 2015
- 年:2015
- 卷:290
- 期:4
- 页码:1207-1229
- 全文大小:5,753 KB
- 参考文献:1. Arge, C.N., Pizzo, V.J. (2000) Improvement in the prediction of solar wind conditions using near-real time solar magnetic field updates. J. Geophys. Res. 105: pp. 10465 g/10.1029/1999JA000262" target="_blank" title="It opens in new window">CrossRef
2. Arge, C.N., Odstrcil, D., Pizzo, V.J., Mayer, L.R. Improved method for specifying solar wind speed near the Sun. In: Velli, M., Bruno, R., Malara, F., Bucci, B. eds. (2003) Tenth Internat. Solar Wind Conf.. AIP, Melvillepp. 190 3. Arge, C.N., Luhmann, J.G., Odstrcil, D., Schrijver, C.J., Li, Y. (2004) Stream structure and coronal sources of the solar wind during the May 12th, 1997 CME. J. Atmos. Solar-Terr. Phys. 66: pp. 1295 g/10.1016/j.jastp.2004.03.018" target="_blank" title="It opens in new window">CrossRef 4. Arge, C.N., Henney, C.J., Koller, J., Compeau, C.R., Young, S., MacKenzie, D., Fay, A., Harvey, J.W. Air force data assimilative photospheric flux transport (ADAPT) model. In: Maksimovic, M., Issautier, K., Meyer-Vernet, N., Moncuquet, M., Pantellini, F. eds. (2010) Twelfth Internat. Solar Wind Conf.. AIP, Melvillepp. 343 5. Arge, C.N., Henney, C.J., Koller, J., Toussaint, W.A., Harvey, J.W., Young, S. Improving data drivers for coronal and solar wind models. In: Pogorelov, N.V., Audit, E., Zank, G.P. eds. (2011) 5th Internat. Conf. Numerical Modeling of Space Plasma Flows. Astron. Soc. Pac., San Franciscopp. 99 6. Brueckner, G.E., Howard, R.A., Koomen, M.J., Korendyke, C.M., Michels, D.J., Moses, J.D., Socker, D.G., Dere, K.P., Lamy, P.L., Llebaria, A., Bout, M.V., Schwenn, R., Simnett, G.M., Bedford, D.K., Eyles, C.J. (1995) The Large Angle Spectroscopic Coronagraph (LASCO). Solar Phys. 162: pp. 357 g/10.1007/BF00733434" target="_blank" title="It opens in new window">CrossRef 7. Burlaga, L.F., Plunkett, S.P., St. Cyr, O.C. (2002) Successive CMEs and complex ejecta. J. Geophys. Res. 107: pp. 1266 g/10.1029/2001JA000255" target="_blank" title="It opens in new window">CrossRef 8. Davies, J.A., Harrison, R.A., Rouillard, A.P., Sheeley, N.R., Perry, C.H., Bewsher, D., Davis, C.J., Eyles, C.J., Crothers, S.R., Brown, D.S. (2009) A synoptic view of solar transient evolution in the inner heliosphere using the heliospheric imagers on STEREO. Geophys. Res. Lett. 36: g/10.1029/2008GL036182" target="_blank" title="It opens in new window">CrossRef 9. Farrugia, C.J., Jordanova, V.K., Thomsen, M.F., Lu, G., Cowley, S.W.H., Ogilvie, K.W. (2006) A two-ejecta event associated with a two-step geomagnetic storm. J. Geophys. Res. 111: g/10.1029/2006JA011893" target="_blank" title="It opens in new window">CrossRef 10. Gopalswamy, N., Yashiro, S., Michalek, G., Kaiser, M.L., Howard, R.A., Reames, D.V., Leske, R., Rosenvinge, T. (2002) Interacting coronal mass ejections and solar energetic particles. Astrophys. J. Lett. 572: pp. L103 g/10.1086/341601" target="_blank" title="It opens in new window">CrossRef 11. Harvey, J.W., Hill, F., Hubbard, H.P., Kennedy, J.R., Leibacher, J.W., Pintar, J.A., Gilman, P.A., Noyes, R.W., Title, A.M., Toomre, J. (1996) The Global Oscillation Network Group (GONG) project. Science 272: pp. 1284 g/10.1126/science.272.5266.1284" target="_blank" title="It opens in new window">CrossRef 12. Henney, C.J., Toussaint, W.A., White, S.M., Arge, C.N. (2012) Forecasting F10.7 with solar magnetic flux transport modeling. Space Weather 10: g/10.1029/2011SW000748" target="_blank" title="It opens in new window">CrossRef 13. Howard, R.A., Moses, J.D., Socker, D.G., Dere, K.P., Cook, J.W. (2002) Sun Earth Connection Coronal and Heliospheric Investigation (SECCHI). Adv. Space Res. 29: pp. 2017 g/10.1016/S0273-1177(02)00147-3" target="_blank" title="It opens in new window">CrossRef 14. Kaiser, M. (2005) The STEREO mission: An overview. Adv. Space Res. 36: pp. 1483 g/10.1016/j.asr.2004.12.066" target="_blank" title="It opens in new window">CrossRef 15. Lee, C.O., Arge, C.N., Odstrcil, D., Millward, G., Pizzo, V. Ensemble modeling of successive halo CMEs observed during 2?–- Aug 2011. In: Zank, G.P., Borovsky, J., Bruno, R., Cirtain, J., Cranmer, S., Elliot, H., Giacalone, J., Gonzalez, W., Li, G., Marsch, E., Moebius, E., Pogorelov, N., Spann, J., Verkhoglyadova, O. eds. (2013) Thirteenth Internat. Solar Wind Conf.. AIP, Melvillepp. 223 16. Lee, C.O., Arge, C.N., Odstrcil, D., Millward, G., Pizzo, V., - 刊物类别:Physics and Astronomy
- 刊物主题:Physics
Astronomy Extraterrestrial Physics and Space Sciences Astrophysics
- 出版者:Springer Netherlands
- ISSN:1573-093X
文摘
The Wang–Sheeley–Arge (WSA)–Enlil cone modeling system is used for making routine arrival-time forecasts of Earth-directed halo coronal mass ejections (CMEs), since they typically produce the most geoeffective events. A major objective of this work is to better understand the sensitivity of the WSA–Enlil modeling results to input model parameters and how these parameters contribute to the overall model uncertainty and performance. In this study, ensemble-modeling results for a succession of three halo CME events that occurred on 2?–- August 2011 are presented. We investigate the sensitivity of the modeled CME arrival times to small variations in the input-cone properties by creating ensemble sets of numerical simulations for each CME event, based on multiple sets of cone parameters. We find that the accuracy of the modeled CME arrival times not only depends on the small variations to the initial input geometry, but also on the reliable specification of the background solar wind, which is driven by the input maps of the photospheric magnetic field. The accuracy in the arrival-time predictions also depends on whether the cone parameters for all three CMEs are specified in a single WSA–Enlil simulation. The inclusion or exclusion of one or two of the preceding CMEs affects the solar-wind conditions through which the succeeding CME propagates. Although the accuracy of the modeled arrival times is sensitive to the input maps that are used to drive the background solar wind, the spread in the modeling ensemble remains mostly unchanged when different input maps are used.
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