Magnetic reconnection in the magnetotail results in the formation of helical or loop-like magnetic structures called plasmoids, which contain strong plasma pressure gradients that maximize along the central axis and balance the magnetic forces directed inward (Hones et al., 1984; Kivelson & Khurana, 1995; Slavin et al., 1989). However, a subset of plasmoids, called "flux-ropes," lack strong pressure gradients in their interior, and the magnetic force of the outer wraps is balanced by the strong axial core field present at their center (Moldwin & Hughes, 1991; Sibeck et al., 1984). Flux ropes in which magnetic stresses are completely self-balancing are referred to as "force-free" as J B p u 0. These force-free flux ropes correspond to the minimum energy state for a plasmoid that all such structures will evolve toward with increasing time (Priest, 2013; Taylor, 1974). Plasmoids which lack a core field and possess weak magnetic fields at their center compared to their surroundings are termed "O-lines." Decades of in situ observations in the terrestrial magnetosphere, together with kinetic simulations (Drake et al., 2006a; Drake et al., 2006b), have revealed that magnetic flux ropes in the night-side plasma sheet can range in size from order 1 to 10 Earth radii (