Altitude dependencies in the solar activity variations of the ionospheric electron density

In this study, 7 years (1986-1992) of measurements from the Japanese middle and upper atmosphere (MU) radar have been analyzed to investigate the solar activity variations of the ionosphere. The observations show strong altitude dependencies in the solar activity variations of the electron density. Below 300 km altitude, the electron density increases nonlinearly with F10.7, with the rate of increase being much lower when F10.7 is greater than 150. This nonlinear variation becomes weaker with increasing altitude. Above 450 km altitude, the electron density increases almost linearly with F10.7 when F10.7 lies in the range 100 to 250. For values of F10.7 less than 100, the electron density at low altitudes increases with increasing F10.7, while at higher altitudes (above about 400 km) the electron density remains almost constant. Mechanisms to explain the observed behavior have been investigated using the Sheffield University Plasmasphere Ionosphere Model. The model calculations show that while the variations with F10.7 of the solar EUV flux and neutral gas densities play important roles in the nonlinear variations of the electron density with F10.7, the correlation of the plasma loss rate with temperature being negative at low temperatures and positive at high temperatures is an important mechanism for the nonlinear variations at low altitudes. Model results also suggest that vibrationally excited N 2 strengthens the nonlinear variations of electron density with F10.7. The disappearance of the nonlinear variations at high altitudes, for values of F10.7 above 100, results from the altitude dependencies of the neutral gas variation on F10.7 and of the relative importance of plasma loss, production, and diffusion processes. At high altitudes, the plasma loss processes, which play an important role in the nonlinear variations at low altitudes, are unimportant when compared with the effects arising from plasma production and diffusion. The altitude dependencies of the electron density variations with F10.7, for values of F10.7 less than 100, are due mainly to the altitude dependencies of the neutral gas densities with F10.7.

[1]  S. Fukao,et al.  Equinoctial asymmetries in the ionosphere and thermosphere observed by the MU radar , 1998 .

[2]  S. Fukao,et al.  New aspects in the annual variation of the ionosphere observed by the MU Radar , 1997 .

[3]  A. Viggiano,et al.  Rate constants for the reactions of O+ with N2 and O2 as a function of temperature (300–1800 K) , 1997 .

[4]  S. Fukao,et al.  Modeling studies of the middle and upper atmosphere radar observations of the ionospheric F layer , 1997 .

[5]  S. Fukao,et al.  Longitudinal variations of the topside ionosphere at low latitudes: Satellite measurements and mathematical modelings , 1996 .

[6]  G. J. Bailey,et al.  Variations of the ionosphere and related solar fluxes during solar cycles 21 and 22 , 1996 .

[7]  R. Moffett,et al.  Vibrational nitrogen concentration in the ionosphere and its dependence on season and solar cycle , 1995 .

[8]  P. Richards,et al.  Ionospheric electron densities calculated using different EUV flux models and cross sections: Comparison with radar data , 1995 .

[9]  S. Watanabe,et al.  Comparison of satellite electron density and temperature measurements at low latitudes with a plasmasphere‐ionosphere model , 1995 .

[10]  S. Fukao,et al.  A Review of MU Radar Observations of the Thermosphere and Ionosphere , 1995 .

[11]  M. Buonsanto Millstone Hill incoherent scatter F region observations during the disturbances of June 1991 , 1995 .

[12]  R. Moffett,et al.  Modeling studies of ionospheric variations during an intense solar cycle , 1994 .

[13]  B. Jenkins,et al.  Variations of ionospheric ionization and related solar fluxes during an intense solar cycle , 1994 .

[14]  T. Tsuda,et al.  Middle and upper atmosphere radar observations of ionospheric electric fields , 1993 .

[15]  G. J. Bailey,et al.  A modelling study of the equatorial topside ionosphere , 1993 .

[16]  H. Rishbeth Day-to-day ionospheric variations in a period of high solar activity , 1993 .

[17]  R. P. Kane Solar cycle variation of ƒoF2 , 1992 .

[18]  W. Kent Tobiska,et al.  Revised solar extreme ultraviolet flux model , 1991 .

[19]  M. Yamamoto,et al.  Measurements of ionospheric and thermospheric temperatures and densities with the middle and upper atmosphere radar , 1991 .

[20]  Ronald F. Woodman,et al.  Average vertical and zonal F region plasma drifts over Jicamarca , 1991 .

[21]  N. W. Spencer,et al.  Revised global model of thermosphere winds using satellite and ground‐based observations , 1991 .

[22]  G. J. Bailey,et al.  A mathematical model of the Earth's plasmasphere and its application in a study of He + at L = 3. , 1990 .

[23]  T. Tsuda,et al.  Ionospheric incoherent scatter measurements with the middle and upper atmosphere radar: Techniques and capability , 1989 .

[24]  A. Hedin MSIS‐86 Thermospheric Model , 1987 .

[25]  P. Richards,et al.  A factor of 2 reduction in theoretical F2 peak electron density due to enhanced vibrational excitation of N2 in summer at solar maximum , 1986 .

[26]  Susumu Kato,et al.  The MU radar with an active phased array system: 2. In‐house equipment , 1985 .

[27]  Susumu Kato,et al.  The MU radar with an active phased array system: 1. Antenna and power amplifiers , 1985 .

[28]  H. Hinteregger,et al.  Observational, reference and model data on solar EUV, from measurements on AE-E , 1981 .

[29]  J. St.‐Maurice,et al.  Erratum: Nonthermal rate coefficients in the ionosphere: the reactions of O+ with N2, O2, and NO , 1978 .

[30]  W. Neupert,et al.  Slowly varying component of extreme ultraviolet solar radiation and its relation to solar radio radiation , 1974 .