Electron and proton radiation belt dynamic simulations during storm periods: A new asymmetric convection-diffusion model

Using a convection-diffusion theory, we give the first results from a four-dimensional model of electron and proton radiation belts. This work is based on the numerical solution of a convection-diffusion equation taking into account (1) for protons, the deceleration of protons by the free and bounded thermospheric and ionospheric electrons, the charge exchange loss process, radial and azimuthal transports, and (2) for electrons, the deceleration of electrons by the free and bounded electrons of the medium, pitch angle diffusion by Coulomb and wave-particle interactions, radial and azimuthal transport. This model allows for simulation of a magnetic storm effects by increasing convective electric field and injecting particles with keV range energies in the nightside region. Particles in the energy range 50 – 100 keV are “created” by acceleration of slower particles in the L = 4 region. Four hours are needed for ring current formation. The calculated particle distribution at 6.6 Earth radii as well as at low altitude are in good agreement with those deduced from ATS 6 measurements (the drift echo is well reproduced at this altitude) and from statistical studies of the precipitation by the DMSP satellites, respectively.

[1]  J. Sauvaud,et al.  Magnetic storm modeling in the Earth's electron belt by the Salammbô code , 1996 .

[2]  T. Moore,et al.  Ring current development during storm main phase , 1996 .

[3]  D. Boscher,et al.  Dynamic modeling of trapped particles , 1996 .

[4]  D. Boscher,et al.  SALAMMBO: A three‐dimensional simulation of the proton radiation belt , 1995 .

[5]  Daniel Boscher,et al.  A three-dimensional analysis of the electron radiation belt by the Salammbô code , 1995 .

[6]  A. Korth,et al.  Long-term observations of keV ion and electron variability in the outer radiation belt from CRRES , 1995 .

[7]  R. Sheldon Ion transport and loss in the Earth's quiet ring current: 2. Diffusion and magnetosphere‐ionosphere coupling , 1994 .

[8]  Margaret W. Chen,et al.  Simulations of phase space distributions of storm time proton ring current , 1994 .

[9]  R. Wolf,et al.  Comparison of diffusion and particle drift descriptions of radial transport in the earth's inner magnetosphere , 1992 .

[10]  R. D. Belian,et al.  Drifting holes in the energetic electron flux at geosynchronous orbit following substorm onset , 1992 .

[11]  R. D. Belian,et al.  Further investigation of the CDAW 7 substorm using geosynchronous particle data: Multiple injections and their implications , 1992 .

[12]  Daniel N. Baker,et al.  Linear prediction filter analysis of relativistic electron properties at 6.6 RE , 1990 .

[13]  Daniel N. Baker,et al.  Extreme energetic particle decreases near geostationary orbit - A manifestation of current diversion within the inner plasma sheet , 1990 .

[14]  S. Krimigis,et al.  On the relationship between the energetic particle flux morphology and the change in the magnetic field magnitude during substorms , 1989 .

[15]  M. S. Gussenhoven,et al.  A statistical model of auroral electron precipitation , 1985 .

[16]  M. Kivelson,et al.  Observation and Modeling of Energetic Particles at Synchronous Orbit on July 29, 1977 , 1982 .

[17]  R. M. Buck,et al.  The dynamics of energetic electrons in the Earth's outer radiation belt during 1968 as observed by the Lawrence Livermore National Laboratory's Spectrometer on Ogo 5 , 1981 .

[18]  W. Spjeldvik Equilibrium structure of equatorially mirroring radiation belt protons , 1977 .

[19]  D. Williams,et al.  The quiet time structure of energetic (35–560 keV) radiation belt electrons , 1975 .

[20]  A. J. Chen,et al.  Isolated cold plasma regions - Observations and their relation to possible production mechanisms , 1975 .

[21]  R. Thorne,et al.  Equilibrium structure of radiation belt electrons , 1973 .

[22]  C. Kennel,et al.  Pitch-angle diffusion of radiation belt electrons within the plasmasphere. , 1972 .

[23]  John M. Cornwall,et al.  Radial diffusion of ionized helium and protons: A probe for magnetospheric dynamics , 1972 .

[24]  M. Walt,et al.  Source and loss processes of protons of the inner radiation belt. , 1971 .

[25]  G. Mead,et al.  Diffusion of protons in the outer radiation belt. , 1965 .

[26]  Carl-Gunne Fälthammar,et al.  Effects of time‐dependent electric fields on geomagnetically trapped radiation , 1965 .

[27]  M. Walt 1. Treatment of Particles with Mirroring Points at High Altitude , 1962 .

[28]  W. Macdonald,et al.  2. Particles with Mirroring Points at Low Altitude , 1962 .

[29]  R. S. White,et al.  Particle fluxes in the inner radiation belt , 1960 .

[30]  M. Schulz,et al.  2 – The Magnetosphere , 1991 .

[31]  M. S. Gussenhoven,et al.  A statistical model of auroral ion precipitation , 1989 .

[32]  D. Williams Phase space variations of near equatorially mirroring ring current ions , 1981 .

[33]  A. Hedin Tables of thermospheric temperature, density and composition derived from satellite and ground based measurements. Volume 2: Ap=20 , 1979 .

[34]  H. Volland A semiempirical model of large‐scale magnetospheric electric fields , 1973 .

[35]  G. W. Sharp,et al.  The Reaction of the Plasmapause to Varying Magnetic Activity , 1970 .

[36]  M. Walt,et al.  Loss Rates of Trapped Electrons by Atmospheric Collisions , 1966 .