Electric field change measurements are a key observation to elucidate the physics of lightning discharges. In particular, slow electric field changes, manifesting over timescales of hundreds of microseconds or longer, are produced by the large-scale motions of charge during leader growth, return strokes, and continuing current (Brook et al., 1962;Kasemir, 1960). Coordinated slow electric field change measurements from multiple sites can be used to estimate the locations and magnitudes of the charge centers involved in lightning discharge processes, which, before the advent of radio frequency lightning mapping systems, provided the means to discern the electric structure of storms and how the propagation of lightning is related to and affected by that structure (Jacobson & Krider, 1976;Krehbiel et al., 1979).In the realm of volcanic lightning, much remains to be learned about how charge is organized in the eruption plume, how it evolves over time, and how it affects the production of lightning. Thomas et al. (2010) showed that the electrical activity during an explosive volcanic eruption transitions through three phases: first, numerous vent discharges, on the order of four meters or less, occur within the gas-thrust region of the plume and produce continual radio frequency impulses (Behnke et al., 2021). Next, near-vent lightning occurs at low altitudes in the eruption column, much of which may connect to ground (Aizawa et al., 2016;Cimarelli et al., 2016). These electrical discharges range from tens of meters (Behnke et al., 2018) up to many kilometers in length (Thomas et al., 2010). Lastly, plume lightning occurs in the convective portion of the plume, and is most similar to thunderstorm lightning (