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Simulating Superstorm Plasma Sources Mei-Ching Fok 1 , Thomas E. Moore 1 , Dominique C. Delcourt 2 Joel A. Fedder 3 , and Steven P. Slinker 4 1 NASA Goddard Space Flight Center, USA 2 Centre d'etude des Environnements Terrestre et Planetaires, France 3 Icarus Research Inc., USA
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Simulating Superstorm Plasma Sources Mei-Ching Fok1, Thomas E. Moore1, Dominique C. Delcourt2 Joel A. Fedder3, and Steven P. Slinker4 1NASA Goddard Space Flight Center, USA 2Centre d'etude des Environnements Terrestre et Planetaires, France 3Icarus Research Inc., USA 4Naval Research Laboratory, USA SM44A-05, May 29, 2008 2008 Joint Assembly Fort Lauderdale, Florida
Global Ion Kinetic Model Solar Wind Parameters LFM Event Run Polar, Auroral Outflow Models Test-Particle Model Solar Wind Particle Distribution Polar Wind Particle Distribution Auroral Wind Particle Distribution Comprehensive Ring Current Model (CRCM) Plasmasphere Model
Global Ion Kinetic Model Solar Wind Parameters LFM Event Run Polar, Auroral Outflow Models Plasmaspheric Outflow Model Test-Particle Model Solar Wind Particle Distribution Polar Wind Particle Distribution Auroral Wind Particle Distribution Comprehensive Ring Current Model (CRCM) Plasmasphere Model
Global Ion Kinetic Model Solar Wind Parameters LFM Event Run Polar, Auroral Outflow Models Plasmaspheric Outflow Model Test-Particle Model Plasmaspheric Wind Particle Distribution Solar Wind Particle Distribution Polar Wind Particle Distribution Auroral Wind Particle Distribution Comprehensive Ring Current Model (CRCM) Plasmasphere Model
Plasmasphere Model Driven by LFM-CRCM Fields CRCM run without plasmaspheric wind particles CRCM run with plasmaspheric wind particles • Plasmapause is closer to the Earth when plasmaspheric wind is not included. • Similar plume structure and escape flux on the dayside for both cases.
Ring Current Total Energy • Similar total energy: SW and AW displaced by PSW • PSW is dominant over SW and AW
Global Ion (H+) Energetics • Enhances total energy • Reduces mean energy of solar wind • Reduces overall mean energy • Suggests two-temperature ring current plasma
Why Is Plasmaspheric-Wind Dominant in Ring Current? Plasmaspheric Wind (PSW) • High PSW density at dusk local times at the CRCM boundary. • Deep penetration of keV’s PsW particles into low L’s Solar Wind (SW)
Conclusions • Plasmaspheric wind (PSW) important, even dominant • PsW “displaces” other sources (CRCM is self-consistent) • But how to detect PSW (THEMIS observed PSW)? Without PSW With PSW