We begin with a derivation of a new physically-based spume generation function to find the drop distribution at the surface. Unlike most previous studies, both the magnitude and shape of this generation function change with wind forcing and sea-state. In addition to reasonable agreement between this spume generation function and the limited data available, we find a potential explanation for the vast drop size differences among previous spume generation studies through a distinction between formed and suspended drops. To calculate the duration of suspension and mean air-drop fluxes, we employ a Lagrangian model to track individual droplets from ejection into the air to ocean reentry or quasi-equilibrium. With this model, we find somewhat different suspension times and individual drop fluxes when solving the full microphysical and transport equations simultaneously. Because of the relative suspension time, the aggregate spume drop fluxes only become significant for intense wind forcing.
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