Modeling the Development of an Equatorial Plasma Bubble During a Midnight Temperature Maximum With SAMI3/WACCM‐X.

We report results from a self‐consistent global simulation model in which a large‐scale equatorial plasma bubble (EPB) forms during a midnight temperature maximum (MTM). The global model comprises the ionospheric code SAMI3 and the atmosphere/thermosphere code WACCM‐X. We consider solar minimum conditions for the month of August. We show that an EPB forms during an MTM in the Pacific sector and is caused by equatorward neutral wind flows. Although this is consistent with the theoretical result that a meridional neutral wind (V) with a negative gradient (∂V/∂θ < 0) is a destabilizing influence [Huba & Krall, 2013, https://doi.org/10.1002/grl.50292] (where a northward meridional neutral wind V is positive and θ is the latitude and increases in the northward direction), we find that the primary cause of the EPB is the large decrease in the Pedersen conductance caused by the equatorward winds. Plain Language Summary: The equatorial ionosphere often develops electron density irregularities at night in the altitude range 300–1,000 km. This phenomenon is known as equatorial spread F. A leading candidate to explain the generation of these irregularities is the generalized Rayleigh‐Taylor instability (GRTI). The phenomenon usually occurs after sunset but under certain conditions it can occur around midnight. In this paper, using the coupled ionosphere/thermosphere model SAMI3/WACCM‐X, we show that it can occur during a midnight temperature maximum where the neutral thermosphere temperature increases near the equator. This is associated with equatorward neutral wind flows that change the conductance of the ionosphere and leads to an increase in the growth rate of the GRTI and the development of a large equatorial plasma bubble. Key Points: An equatorial plasma bubble can develop during a midnight temperature maximum in the ionosphereEquatorward winds reduce the Pedersen conductance that enhances the growth rate of the generalized Rayleigh‐Taylor instabilityThe results are based on the coupled ionosphere/thermosphere model SAMI3/WACCM‐X [ABSTRACT FROM AUTHOR]