Abstract

Abstract. We have combined ~300 h of tristatic measurements of the field-perpendicular F region ionospheric flow measured overhead at Tromsø by the EISCAT UHF radar, with simultaneous IMP-8 measurements of the solar wind and interplanetary magnetic field (IMF) upstream of the Earth's magnetosphere, in order to examine the response time of the ionospheric flow to changes in the north-south component of the IMF (Bz). In calculating the flow response delay, the time taken by field changes observed by the spacecraft to first effect the ionosphere has been carefully estimated and subtracted from the response time. Two analysis methods have been employed. In the first, the flow data were divided into 2 h-intervals of magnetic local time (MLT) and cross-correlated with the "half-wave rectifier" function V2Bs, where V is the solar wind speed, and Bs is equal to IMF Bz if the latter is negative, and is zero otherwise. Response delays, determined from the time lag of the peak value of the cross-correlation coefficient, were computed versus MLT for both the east-west and north-south components of flow. The combined data set suggests minimum delays at ~1400 MLT, with increased response times on the nightside. For the 12-h sector centred on 1400 MLT, the weighted average response delay was found to be 1.3 ± 0.8 min, while for the 12-h sector centred on 0200 MLT the weighted average delay was found to increase to 8.8 ± 1.7 min. In the second method we first inspected the IMF data for sharp and enduring (at least ~5 min) changes in polarity of the north-south component, and then examined concurrent EISCAT flow data to determine the onset time of the corresponding enhancement or decay of the flow. For the case in which the flow response was timed from whichever of the flow components responded first, minimum response delays were again found at ~1400 MLT, with average delays of 4.8 ± 0.5 min for the 12-h sector centred on 1400 MLT, increasing to 9.2 ± 0.8 min on the nightside. The response delay is thus found to be reasonably small at all local times, but typically ~6 min longer on the nightside compared with the dayside. In order to make an estimate of the ionospheric information propagation speed implied by these results, we have fitted a simple theoretical curve to the delay data which assumes that information concerning the excitation and decay of flow propagates with constant speed away from some point on the equatorward edge of the dayside open-closed field line boundary, taken to lie at 77° magnetic latitude. For the combined cross-correlation results the best-fit epicentre of information propagation was found to be at 1400 MLT, with an information propagation phase speed of 9.0 km s–1. For the combined event analysis, the best-fit epicentre was also found to be located at 1400 MLT, with a phase speed of 6.8 km s–1.Key words. Interplanetary physics (interplanetary magnetic fields) · Magnetospheric physics (Plasma convection; solar wind · magnetosphere interactions)

Highlights

  • Observations of plasma convection in the high-latitude ionosphere by polar-orbiting satellites have demonstrated that the form and magnitude of theow depends on the direction and strength of the interplanetary magnetic®eld (IMF) which impinges on the dayside magnetopause boundary of the Earth's magnetosphere (e.g.Heppner, 1972; Rei€ et al, 1981; Rei€ and Burch, 1985)

  • Two regimes are evident, corresponding to the region of negative correlations indicated by the square symbols, which span the dayside east-westow reversal centred on 0900±1000 magnetic local time (MLT), and a region of positive correlations indicated by the circles, which are observed in the dusk and early evening sector

  • We have compared 300 simultaneous hours of observations of the high-latitude ionosphericow obtained by the EISCAT UHF radar with measurements of the interplanetary ®eld made by the IMP-8 spacecraft upstream from the Earth's magnetosphere, in order to determine the time scale on which the ionosphericow responds to changes in the north-south component of the IMF

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Summary

Introduction

®eld (IMF) which impinges on the dayside magnetopause boundary of the Earth's magnetosphere Based on these observations, Cowley and Lockwood (1992, 1997) have suggested a theoretical picture in whichow changes occurring in response to variations in the direction of the IMF begin in the dayside cusp near noon, and propagate away from this vicinity to establish a new steady-state convection pattern over intervals of 10±15 min. This expansion of theow pattern corresponds to the ionospheric image of the expansion of the perturbedow region at large distances in the magnetosphere. The 2-min averagedow data employed here should be capable of distinguishing between these possibilities and of resolving day-night di€erences of this order, though only just so for phase speeds at the top end of the range considered likely

Instrumentation and data sets
The EISCAT CP-1-K experiment
IMP-8 interplanetary data
The combined data set
Cross-correlation analysis
Event analysis
Summary and discussion
Full Text
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