Energetic particle penetrations into the inner magnetosphere

Data from Explorer 45 (S³-A) instruments have revealed characteristics of magnetospheric storm or substorm time energetic particle enhancements in the inner magnetosphere (L ≲5). The properties of the ion ‘nose’ structure in the dusk hemisphere are examined in detail. A statistical study of the local time dependence of noses places the highest probability of occurrence around 2000 MLT, but they can be observed even near the noon meridian. It also appears that most noses are not isolated events but will appear on successive passes. A geoelectric field enhancement corresponding to a minimum value of AE of about 205 γ seems to be required to convect the particles within the apogee of Explorer 45. The dynamical behavior of the nose characteristics observed along successive orbits is then explained quantitatively by the time-dependent convection theory in a Volland-Stern type geoelectric field (γ=2). These calculations of adiabatic charged particle motions are also applied to explain the energy spectra and dispersion in penetration distances for both electrons and ions observed in the postmidnight to morning hours. Finally, useful descriptions are given of the dispersion properties of particles penetrating the inner magnetosphere at all local times as a function of time after a sudden enhancement of the geoelectric field.

[1]  A. J. Chen Penetration of low‐energy protons deep into the magnetosphere , 1970 .

[2]  Ejiri,et al.  Trajectory traces of charged particles in the magnetosphere. [1 to keV] , 1976 .

[3]  R. Hoffman,et al.  Direct observations in the dusk hours of the characteristics of the storm-time ring current particles during the beginning of magnetic storms , 1974 .

[4]  C. Mcilwain,et al.  PLASMA CLOUDS IN THE MAGNETOSPHERE. , 1971 .

[5]  C. Mcilwain,et al.  The onset time of magnetospheric substorms determined from ground and synchronous satellite records , 1974 .

[6]  S. B. Mende,et al.  Plasma Injection at Synchronous Orbit and Spatial and Temporal Auroral Morphology , 1976 .

[7]  J. Grebowsky,et al.  Effects of convection electric field on the distribution of ring current type protons , 1975 .

[8]  T. Fritz,et al.  Injection boundary dynamics during a geomagnetic storm , 1976 .

[9]  G. Parks,et al.  Acceleration of energetic electrons observed at the synchronous altitude during magnetospheric substorms. , 1968 .

[10]  E. W. Hones,et al.  Motion of magnetospheric particle clouds in a time-dependent electric field model , 1974 .

[11]  M. Kivelson Magnetospheric electric fields and their variation with geomagnetic activity , 1976 .

[12]  T. Fritz,et al.  Substorm‐injected protons and electrons and the injection boundary model , 1975 .

[13]  R. Hoffman,et al.  The convection electric field model for the magnetosphere based on Explorer 45 observations , 1978 .

[14]  B. Mauk,et al.  Correlation of Kp with the substorm‐injected plasma boundary , 1974 .

[15]  G. W. Longanecker,et al.  S³‐A spacecraft and experiment description , 1973 .

[16]  M. Kivelson,et al.  Time dependent convection electric fields and plasma injection. [to inner magnetosphere , 1979 .

[17]  N. Maynard,et al.  Double floating probe measurements on S³‐A , 1973 .

[18]  R. Hoffman,et al.  Inference of the ring current ion composition by means of charge exchange decay , 1981 .