Abstract
It is well known that the polar cap, delineated by the Open Closed field line Boundary (OCB), responds to changes in the Interplanetary Magnetic Field (IMF). In general, the boundary moves equatorward when the IMF turns southward and contracts poleward when the IMF turns northward. However, observations of the OCB are spotty and limited in local time, making more detailed studies of its IMF dependence difficult. Here, we simulate five solar storm periods with the coupled model consisting of the Open Geospace General Circulation model (OpenGGCM) coupled with Coupled Thermosphere Ionosphere Model (CTIM) and the Rice Convection Model (RCM), i.e., the OpenGGCM-CTIM-RCM model, to estimate the location and dynamics of the OCB. For these events, polar cap boundary location observations are also obtained from Defense-Meteorological Satellite Program (DMSP) precipitation spectrograms and compared with the model output. There is a large scatter in the DMSP observations and in the model output. However, we generally find good agreement between the model and the observations. On average, the model overestimates the latitude of the open-closed field line boundary by 1.61 degrees. Additional analysis of the simulated polar cap boundary dynamics across all local times shows that the MLT of the largest polar cap expansion closely correlates with the IMF clock angle; that the strongest correlation occurs when the IMF is southward; that during strong southward IMF the polar cap shifts sunward; and that the polar cap rapidly contracts at all local times when the IMF turns northward.
Highlights
The total magnetic flux contained in the open magnetic field lines of Earth’s polar caps is a crucial parameter for the energy stored in the magnetosphere, and for substorm and storm dynamics (Siscoe and Huang, 1985; Milan et al, 2008)
Additional analysis of the simulated polar cap boundary dynamics across all local times shows that the Magnetic Local Time (MLT) of the largest polar cap expansion closely correlates with the Interplanetary Magnetic Field (IMF) clock angle; that the strongest correlation occurs when the IMF is southward; that during strong southward IMF the polar cap shifts sunward; and that the polar cap rapidly contracts at all local times when the IMF 15 turns northward
Before we consider a detailed analysis of the simulation runs, we first assess the realism of the simulations by comparing the model Open Closed field line Boundary (OCB) latitude output with Defense-Meteorological Satellite Program (DMSP) observations
Summary
The total magnetic flux contained in the open magnetic field lines of Earth’s polar caps is a crucial parameter for the energy stored in the magnetosphere, and for substorm and storm dynamics (Siscoe and Huang, 1985; Milan et al, 2008). The amount of the open flux is essentially given by the polar cap area, which is bounded by the OCB. The shape and dynamics of 20 the OCB are controlled by magnetic reconnection and large-scale convection (Cowley, 1982; Milan et al, 2007). Magnetic flux enters and exits the polar cap through reconnection at the magnetopause and in the tail. Convection can change the shape of the OCB without changing the flux contained in the polar cap.
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