The transport of ions from the ionosphere and into the magnetosphere, known as "ionospheric outflow" or "ion outflow," has many implications for Earth's magnetospheric composition and dynamics. Plasma in the magnetosphere resulting from ionospheric outflow is found to alter magnetic reconnection (e.g., Karimabadi et al., 2011;Shay et al., 2004), change the flows in the magnetotail (e.g., Brambles et al., 2011;Garcia et al., 2010), and impact the inner magnetosphere (e.g., Moore et al., 2005;Welling et al., 2011). Moreover, the ionosphere is at times found to be a dominant source of magnetospheric plasma, particularly during geomagnetic storms (Lennartsson et al., 1981) and is arguably a fully adequate source of near-Earth plasma (Chappell et al., 1987;Huddleston et al., 2005). Given the importance of ion outflow to the magnetosphere, it is critical to understand how energy input to the ionosphere drives ionospheric outflow.Energy input in the form of electromagnetic energy and particle precipitation has been shown in observations to be associated with the generation of ion outflows. In particular, statistical studies using data from the POLAR spacecraft (Zheng et al., 2005) and the Fast Auroral SnapshoT (FAST) spacecraft (Strangeway et al., 2005) found a strong correlation between ion outflow flux, Poynting flux, and soft electron precipitation. In these studies, energy inputs and ion outflows were compared at high attitudes, far above the source region of the ion escape. Earlier observations from the Dynamics Explorer (DE) 2 spacecraft also found a connection between soft electron precipitation and ion upflows above the aurora (Seo et al., 1997). Interestingly, the studies of Zheng et al. (2005) and Strangeway et al. (2005) focus on the DC, or quasi-static, Poynting flux. The DC Poynting flux is associated with the large scale convection which can influence ion outflow by generating ion upwelling driven by frictional heating of the ion gas. While much of this heating occurs in the E-region, large amounts are also possible in the F-region (Killeen & Roble, 1984) which can then generate significant transient ion upwelling in the cusp and auroral regions (Gombosi & Killeen, 1987). Similarly, soft electron precipitation can heat the thermal electron population and generate secondary electrons which can enhance the ambipolar electric field and thus lift ionospheric plasma to higher altitudes (Su et al., 1999). The upwelling of plasma caused by either of these processes was speculated by Strangeway et al. (2005) as the first step of the causal chain explaining ion outflow with subsequent wave-particle interactions (WPI) being required to further accelerate the ions to create the energized outflow observed by FAST and POLAR. The online supplemental materials for Brambles et al. ( 2011) expands