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dc.contributor.authorTsurutani, Bruce T.
dc.contributor.authorLakhina, G.S.
dc.contributor.authorEcher, Ezequiel
dc.contributor.authorHajra, Rajkumar
dc.contributor.authorNayak, Chinmaya
dc.contributor.authorMannucci, Anthony J.
dc.contributor.authorMeng, Xing
dc.date.accessioned2011-03-13T01:42:23Z
dc.date.accessioned2021-02-12T10:15:06Z
dc.date.available2011-03-13T01:42:23Z
dc.date.available2021-02-12T10:15:06Z
dc.date.issued2018
dc.identifier.citationGeophysical Research, 123, 1388–1392, doi: 10.1002/ 2017JA024779en_US
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/1207
dc.description.abstractAn alternative scenario to the Ngwira et al. (2014, https://doi.org/10.1002/2013JA019661) high sheath densities is proposed for modeling the Carrington magnetic storm. Typical slow solar wind densities (~5 cm 3) and lower interplanetary magnetic cloud magnetic field intensities (~90 nT) can be used to explain the observed initial and main phase storm features. A second point is that the fast storm recovery may be explained by ring current losses due to electromagnetic ion cyclotron wave scattering. Plain Language Summary The 1859 Carrington magnetic storm is the largest storm in recorded history. It is used as a model of an "extreme storm" by the U.S. Homeland Security for effects of such an event on the U.S. population. Computer modelers have tried to duplicate the magnetic ground signatures of the storm that were published in Tsurutani et al. (2003, https://doi.org/10.1029/2002JA009504). Some have used extremely high solar wind densities, values which have never been detected in the space age. Here we explain why assumptions of such high densities are unnecessary.en_US
dc.language.isoen_USen_US
dc.subjectMagnetic stormsen_US
dc.subjectSolar winden_US
dc.titleComment on “Modeling Extreme “Carrington-Type” Space Weather Events Using Three-Dimensional Global MHD Simulations” by C. M. Ngwira, A. Pulkkinen, M. M. Kuznetsova, and A. Glocer”en_US
dc.typeArticleen_US
dc.identifier.accession091741
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