Abstract

Abstract. Central polar cap convection changes associated with southward turnings of the Interplanetary Magnetic Field (IMF) are studied using a chain of Canadian Advanced Digital Ionosondes (CADI) in the northern polar cap. A study of 32 short duration (~1 h) southward IMF transition events found a three stage response: (1) initial response to a southward transition is near simultaneous for the entire polar cap; (2) the peak of the convection speed (attributed to the maximum merging electric field) propagates poleward from the ionospheric footprint of the merging region; and (3) if the change in IMF is rapid enough, then a step in convection appears to start at the cusp and then propagates antisunward over the polar cap with the velocity of the maximum convection. On the nightside, a substorm onset is observed at about the time when the step increase in convection (associated with the rapid transition of IMF) arrives at the polar cap boundary.Key words: Ionosphere (plasma convection; polar ionosphere) - Magnetospheric physics (solar wind - magnetosphere interaction)

Highlights

  • A number of observations over the past two decades have shown that the plasmaow in the Earth's polar ionosphere is driven by the solar wind-magnetosphericionospheric coupling

  • We ®nd that the central polar cap convection changes associated with short duration southward turning of Interplanetary Magnetic Field (IMF) has 3 components: (1) an initial response to a southward transition that is nearly simultaneous for the entire polar cap, (2) a peak of convection speed that propagates poleward from the ionospheric footprint of the merging region and, if the change in IMF is rapid enough, and (3) a step in convection that appears to start at the cusp and propagates antisunward over the polar cap with velocity of the maximum convection

  • In the previous section we have described the changes in convection at a central polar cap station in response to a southward turning of the IMF

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Summary

Introduction

A number of observations over the past two decades have shown that the plasmaow in the Earth's polar ionosphere is driven by the solar wind-magnetosphericionospheric coupling. Most of the previous studies (Todd et al, 1998; Etamadai et al, 1988; Saunders et al, 1992; Ridley et al, 1998; Ruohoniemi and Greenwald, 1998) were either con®ned to auroral regions (closed ®eld lines) or regions near to the polar cap boundary Some of these have shown that the high-latitude convection responds with a delay after southward transition of IMF (Etamadi et al, 1988; Todd et al, 1988), there are signi®cant di€erences in the measured delays. The exact nature of theow response is a subject of debate (Lockwood and Cowley, 1999; Ridley et al, 1999) Based on these previous studies, there are two schools of thought pertaining to the ionospheric convection response to the southward transition of IMF. We ®nd that the central polar cap convection changes associated with short duration southward turning of IMF has 3 components: (1) an initial response to a southward transition that is nearly simultaneous for the entire polar cap, (2) a peak of convection speed (attributed to the maximum merging electric ®eld) that propagates poleward from the ionospheric footprint of the merging region and, if the change in IMF is rapid enough, and (3) a step in convection that appears to start at the cusp and propagates antisunward over the polar cap with velocity of the maximum convection

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