Pressure changes associated with substorm depolarization in the near-Earth plasma sheet

We have studied plasma (ion) pressure changes that occurred in association with the dipolarization in the near‐Earth plasma sheet around substorm onsets. Using Geotail data, we have performed a superposed epoch analysis in addition to detailed examinations of two individual cases with special emphas...

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Published inJournal of Geophysical Research: Space Physics Vol. 115; no. A12
Main Authors Miyashita, Y., Machida, S., Ieda, A., Nagata, D., Kamide, Y., Nosé, M., Liou, K., Mukai, T., Christon, S. P., Russell, C. T., Shinohara, I., Saito, Y.
Format Journal Article
LanguageEnglish
Published Blackwell Publishing Ltd 01.12.2010
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ISSN0148-0227
2156-2202
DOI10.1029/2010JA015608

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Summary:We have studied plasma (ion) pressure changes that occurred in association with the dipolarization in the near‐Earth plasma sheet around substorm onsets. Using Geotail data, we have performed a superposed epoch analysis in addition to detailed examinations of two individual cases with special emphasis on the contribution of high‐energy particles to the plasma pressure. It is found that, unlike previously reported results, the plasma pressure does increase in association with the initial dipolarization at X > ∼−12 RE and −2 < Y < 6 RE, with the increase largely due to high‐energy particles. Outside the initial dipolarization region, particularly tailward and duskward of this region, the plasma pressure begins to decrease owing to the magnetic reconnection before onset or before the dipolarization region reaches there. At later times, the plasma pressure tends to increase there, related to the expanding dipolarization region, but the contribution of high‐energy particles is not very large. These observations suggest the following. The rarefaction wave scenario proposed in the current disruption model is questionable. The radial and azimuthal pressure gradients may strengthen between the initial dipolarization and outside regions, possibly resulting in stronger braking of fast earthward flows and changes in field‐aligned currents. The characteristics of the dipolarization may differ between the initial dipolarization and tailward regions, which would be possibly reflected in the auroral features. Furthermore, we have examined the specific entropy and the ion β. The specific entropy increases in the plasma sheet in the dipolarization region as well as in the midtail region in conjunction with substorm onsets, suggesting from the ideal MHD point of view that the substorm processes are nonadiabatic. The ion β is found to peak at the magnetic equator in the initial dipolarization region around dipolarization onsets.
Bibliography:istex:F4CB104576B33652F314F9CC43E5BC4EB2D479BB
ArticleID:2010JA015608
ark:/67375/WNG-0QRGZBML-7
ISSN:0148-0227
2156-2202
DOI:10.1029/2010JA015608