Abstract

Abstract. We report and discuss interesting observations of the variability of electric fields and ionospheric densities near sunrise in the equatorial ionosphere made by instruments onboard the Communications/Navigation Outage Forecasting System (C/NOFS) satellite over six consecutive orbits. Electric field measurements were made by the Vector Electric Field Instrument (VEFI), and ionospheric plasma densities were measured by Planar Langmuir Probe (PLP). The data were obtained on 17 June 2008, a period of solar minimum conditions. Deep depletions in the equatorial plasma density were observed just before sunrise on three orbits, for which one of these depletions was accompanied by a very large eastward electric field associated with the density depletion, as previously described by de La Beaujardière et al. (2009), Su et al. (2009) and Burke et al. (2009). The origin of this large eastward field (positive upward/meridional drift), which occurred when that component of the field is usually small and westward, is thought to be due to a large-scale Rayleigh–Taylor process. On three subsequent orbits, however, a distinctly different, second type of relationship between the electric field and plasma density near dawn was observed. Enhancements of the eastward electric field were also detected, one of them peaking around 3 mV m−1, but they were found to the east (later local time) of pre-dawn density perturbations. These observations represent sunrise enhancements of vertical drifts accompanied by eastward drifts such as those observed by the San Marco satellite (Aggson et al., 1995). Like the San Marco measurements, the enhancements occurred during winter solstice and low solar flux conditions in the Pacific longitude sector. While the evening equatorial ionosphere is believed to present the most dramatic examples of variability, our observations exemplify that the dawn sector can be highly variable as well.

Highlights

  • The pre-reversal enhancement (PRE) in the eastward electric field component near sunset in the equatorial ionosphere is a phenomenon that has been well reported and studied

  • Rishbeth (1971) first suggested that the PRE would be a result of charge accumulation below and above the equatorial ionospheric F region that would result from the disappearance of conjugate E region conductivities, and an eastward thermospheric wind

  • Farley et al (1986) explained the PRE as a result of a gradient in the off-equatorial Hall conductivity, coupled with the action of eastward thermospheric neutral winds, which would result into a polarization eastward electric field near sunset

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Summary

Introduction

The pre-reversal enhancement (PRE) in the eastward electric field component near sunset in the equatorial ionosphere is a phenomenon that has been well reported and studied (see Kelley, 2009). The panels are the same as before, here, the grey shadow overlaid on the Earth in the lowest panel corresponds to where the terminator occurs at 100 km altitude Inspection of these six orbits reveals two different general relationships between the electric field and plasma density near dawn. The large electric field enhancement and deep plasma depletion were found before E region sunrise and were anti-correlated; that is, the upward drift had a waveform similar to the density depletion. The E × B enhancements were comparable to the drifts near noon and, on Orbit 918, the component reached 150 m s−1 (∼ 3 mV m−1), certainly among the larger upwards drift amplitudes (zonal equatorial fields) ever measured in the low-latitude ionospheric F region not associated with a density depletion.

A large-scale Rayleigh–Taylor process – Orbit 915
Post-sunrise electric field enhancements – orbits 917–919
Conclusions
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