Propagation of Pi2 pulsations through the braking region in global MHD simulations

dc.contributor.authorReam, J. B.
dc.contributor.authorWalker, R. J.
dc.contributor.authorAshour-Abdalla, M.
dc.contributor.authorEl-Alaoui, M.
dc.contributor.authorWiltberger, M.
dc.contributor.authorKivelson, M. G.
dc.contributor.authorGoldstein, Melvyn
dc.date.accessioned2024-01-17T11:31:34Z
dc.date.available2024-01-17T11:31:34Z
dc.date.issued2015-12-13
dc.description.abstractWe investigate the propagation of Pi2 period pulsations from their origin in the plasma sheet through the braking region, the region where the fast flows are slowed as they approach the inner edge of the plasma sheet. Our approach is to use both the University of California, Los Angeles (UCLA) and Lyon-Fedder-Mobarry (LFM) global magnetohydrodynamic (MHD) computer codes to simulate the Earth's magnetosphere during a substorm that occurred on 14 September 2004 when Pi2 pulsations were observed. We use two different MHD models in order to test the robustness of our conclusions about Pi2. The simulations are then compared with ground-based and satellite data. We find that the propagation of the pulsations in the simulations, especially through the braking region, depends strongly on the ionospheric models used at the inner boundary of the MHD models. With respect to typical observed values, the modeled conductances are high in the UCLA model and low in the LFM model. The different conductances affect the flows, producing stronger line tying that slows the flow in the braking region more in the UCLA model than in the LFM model. Therefore, perturbations are able to propagate much more freely into the inner magnetosphere in the LFM results. However, in both models Pi2 period perturbations travel with the dipolarization front (DF) that forms at the earthward edge of the flow channel, but as the DF slows in the braking region, −8≤x≤−6 RE, the Pi2 period perturbations begin to travel ahead of it into the inner magnetosphere. This indicates that the flow channels generate compressional waves with periods that fall within the Pi2 range and that, as the flows themselves are stopped in the braking region, the compressional wave continues to propagate into the inner magnetosphere.
dc.description.sponsorshipThis work was supported by NASA grant NNX09AV91G. This research was also supported in part by the NASA Graduate Student Research Program through Goddard Space Flight Center, grant NNX10AM08H. M.L. Goldstein and M. Ashour-Abdalla were supported by the Magnetospheric Multiscale project through an Interdisciplinary Science grant to the Goddard Space Flight Center and UCLA (NASA grant NNX08AO48G at UCLA). M. El-Alaoui was supported by NSF grant AGS-1265967. M.G. Kivelson was supported by NASA grant UCB/NASA NAS 5-02099. M. Wiltberger was supported by NASA grant NNX13AE39G. The National Center for Atmospheric Research is sponsored by the National Science Foundation. We would like to acknowledge high-performance computing support from Yellowstone (ark:/85065/d7wd3xhc) provided by NCAR's Computational and Information Systems Laboratory, sponsored by the National Science Foundation. Computational resources for the UCLA model were provided by the Extreme Science and Engineering Discovery Environment (XSEDE), which is supported by National Science Foundation grant OCI-1053575. All satellite and OMNI data were obtained through the Virtual Magnetospheric Observatory (VMO) (http://vmo.igpp.ucla.edu/). We acknowledge the experiment teams that acquired, processed, and provided the OMNI-included data, and J.H. King and N.E. Papitashvili of NASA/GSFC for creating the OMNI data set. Geotail magnetic field data were provided by T. Nagai, JAXA in Japan. We acknowledge C. Carr and the Double Star TC1 FGM instrument team, as well as ESA, Double Star, Center for Space Science and Applied Research, and the Chinese Academy of Sciences for Double Star data. We also acknowledge the World Data Center for Geomagnetism, Kyoto (http://wdc.kugi.kyoto-u.ac.jp/index.html) and the Geomagnetic Network of China, for Pi2 data. We thank Krishan Khurana, Tung-Shin Hsu, and Robert J. Strangeway for helpful discussions during the course of this research.
dc.description.urihttps://agupubs.onlinelibrary.wiley.com/doi/10.1002/2015JA021572
dc.format.extent18 pages
dc.genrejournal articles
dc.identifier.citationReam, J. B., Walker, R. J., Ashour-Abdalla, M., El-Alaoui, M., Wiltberger, M., Kivelson, M. G., and Goldstein, M. L. (2015), Propagation of Pi2 pulsations through the braking region in global MHD simulations, J. Geophys. Res. Space Physics, 120, 10,574–10,591, doi:10.1002/2015JA021572.
dc.identifier.urihttps://doi.org/10.1002/2015JA021572
dc.identifier.urihttp://hdl.handle.net/11603/31313
dc.language.isoen_US
dc.publisherAGU
dc.relation.isAvailableAtThe University of Maryland, Baltimore County (UMBC)
dc.relation.ispartofUMBC Goddard Planetary Heliophysics Institute (GPHI)
dc.relation.ispartofUMBC Faculty Collection
dc.rightsThis work was written as part of one of the author's official duties as an Employee of the United States Government and is therefore a work of the United States Government. In accordance with 17 U.S.C. 105, no copyright protection is available for such works under U.S. Law.
dc.rightsPublic Domain Mark 1.0 en
dc.rights.urihttps://creativecommons.org/publicdomain/mark/1.0/
dc.titlePropagation of Pi2 pulsations through the braking region in global MHD simulations
dc.typeText
dcterms.creatorhttps://orcid.org/0000-0002-5317-988X

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