4.3 Article

Modeling ring current ion and electron dynamics and plasma instabilities during a high-speed stream driven storm

Journal

Publisher

AMER GEOPHYSICAL UNION
DOI: 10.1029/2011JA017433

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Funding

  1. U. S. Department of Energy
  2. NASA [NNH09AL06I, NNX11AJ34G]
  3. NSF [ATM-0902941]
  4. NASA [143721, NNX11AJ34G] Funding Source: Federal RePORTER

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The temporal and spatial development of the ring current is evaluated during the 23-26 October 2002 high-speed stream (HSS) storm, using a kinetic ring current-atmosphere interactions model with self-consistent magnetic field (RAM-SCB). The effects of nondipolar magnetic field configuration are investigated on both ring current ion and electron dynamics. As the self-consistent magnetic field is depressed at large (>4R(E)) radial distances on the nightside during the storm main phase, the particles' drift velocities increase, the ion and electron fluxes are reduced and the ring current is confined closer to Earth. In contrast to ions, the electron fluxes increase closer to Earth and the fractional electron energy reaches similar to 20% near storm peak due to better electron trapping in a nondipolar magnetic field. The ring current contribution to Dst calculated using Biot-Savart integration differs little from the DPS relation except during quiet time. RAM-SCB simulations underestimate vertical bar SYM-H vertical bar minimum by similar to 25% but reproduce very well the storm recovery phase. Increased anisotropies develop in the ion and electron velocity distributions in a self-consistent magnetic field due to energy dependent drifts, losses, and dispersed injections. There is sufficient free energy to excite whistler mode chorus, electromagnetic ion cyclotron (EMIC), and magnetosonic waves in the equatorial magnetosphere. The linear growth rate of whistler mode chorus intensifies in the postmidnight to noon sector, EMIC waves are predominantly excited in the afternoon to midnight sector, and magnetosonic waves are excited over a broad MLT range both inside and outside the plasmasphere. The wave growth rates in a dipolar magnetic field have significantly smaller magnitude and spatial extent.

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