Magnetic reconnection represents a fundamental mode of energy transfer into and out of the geospace system. Many phenomena of the polar ionosphere may be directly traced to reconnection, including the formation of fast flow channels (Zou et al., 2015), poleward moving auroral forms (Oksavik et al., 2004), poleward boundary intensifications (PBI's) along the nightside separatrix (De la Beaujardiere et al., 1994;Zou et al., 2016), and ionospheric upflow in the cusp (Strangeway et al., 2000) and nightside auroral regions (Semeter et al., 2003). From an energy perspective, the merging of the solar wind and magnetosphere constitutes a magnetospheric generator, establishing the electric fields that drive complex convection patterns in the ionosphere. For periods of southward interplanetary magnetic field (IMF), observational evidence suggests that, on average, there is a balance between magnetopause reconnection on the dayside and magnetotail reconnection on the nightside (Dungey, 1961). When the IMF is northward directed, reconnection occurs differently from the southward IMF. Regions that are favorable to reconnection shift from the dayside magnetopause to the lobe magnetic field lines poleward of the cusps (Gosling et al., 1991). The formation of reverse convection cells, multi-cell convection patterns, and soft discrete arcs in the polar cap are some of the consequences that arise due to the reversal in orientation of the IMF B z component from negative (southward) to positive (northward) (