Fig. 1 | npj Climate and Atmospheric Science

Fig. 1

From: Observational constraint of in-cloud supersaturation for simulations of aerosol rainout in atmospheric models

Fig. 1The alternative text for this image may have been generated using AI.

Conceptual diagram of the BC tracer method. The mass-equivalent diameter (Dtr) of each water-insoluble BC particle is an observable invariant during removal and transport processes. In a convective-type precipitating cloud system, the removal efficiency of aerosols in a moist air parcel uplifted from the boundary layer is determined mainly by the nucleation scavenging process within each localized supersaturated domain (LSD). The occurrence and activity of LSDs in a cloud system are complex functions of time and space. For simplicity, the figure illustrates a temporal snapshot of the spatial distribution of discrete LSDs (LSDk, k = 1, …, n). For each rainfall event, the average of SSlsd, weighted by the number of tracer particles scavenged in LSDk (k = 1, …, n), is estimated by comparing the Dtr-resolved number concentrations of initial tracer (in the surface air) and removed tracer (in rainwater) measured at a surface observation site. For each rainfall event, the rainwater sampling period was typically ~100−101 min (Table S1). The cloud system moves horizontally ~100−101 km during the rainwater sampling under the typical wind speed in the lower troposphere of ~10 ms–1. The number (n) of LSDs contributing to the scavenging of observed tracer depends on the sampling period as well as on the translational speed of the cloud system

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