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Spatial distribution of relative humidity (colour-coded) and horizontal wind (arrows) at 950 hPa at 14:00 UTC (a) and 21:00 UTC (b) averaged for the months of July and August 2006. Data are from the 2.8 km simulation.  

Spatial distribution of relative humidity (colour-coded) and horizontal wind (arrows) at 950 hPa at 14:00 UTC (a) and 21:00 UTC (b) averaged for the months of July and August 2006. Data are from the 2.8 km simulation.  

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We performed a high-resolution numerical simulation to study the development of extensive low-level clouds that frequently form over southern West Africa during the monsoon season. This study was made in preparation for a field campaign in 2016 within the Dynamics-aerosol-chemistry-cloud interactions in West Africa (DACCIWA) project and focuses on...

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Context 1
... front occurs regularly when an undisturbed south-westerly monsoon flow prevails along the coast and further inland. Figure 5 shows the relative humidity at 950 hPa averaged for the 2 months. The front evolves along the coast after noon, which is re- flected by a strong gradient in relative humidity between the relatively cool maritime air mass over the Gulf of Guinea and warmer air over land (Fig. 5a). ...
Context 2
... monsoon flow prevails along the coast and further inland. Figure 5 shows the relative humidity at 950 hPa averaged for the 2 months. The front evolves along the coast after noon, which is re- flected by a strong gradient in relative humidity between the relatively cool maritime air mass over the Gulf of Guinea and warmer air over land (Fig. 5a). In general, moisture increases from south to north, which is related to strong evaporation over land. Within this large-scale moisture difference a local maximum exists along the front. This is caused by moisture convergence and upward transport of moisture from close to the surface when the monsoon flow decelerates due to surface ...
Context 3
... the coast. During the afternoon, the front is rather stationary, located about 30 km inland along the coast of eastern Ghana, Togo and western Benin. Further to the east, the front is more diffuse and is located farther away from the coast. After 16:00 UTC, the front starts pen- etrating inland and reaches SAVE at around 21:00 UTC on the average (Fig. 5b), which agrees well with the conditions of the case study (Figs. 3a, e and 4). During the subsequent hours, the front becomes more diffuse on the average, but continues to propagate ...

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Within the framework of the DACCIWA (Dynamics-Aerosol-Chemistry-Cloud-Interactions over West Africa) project, and based on a field experiment conducted in June and July 2016, we analyse the daytime breakup of the continental low-level stratiform clouds in southern West Africa. We use the observational data gathered during twenty-two precipitation-free occurrences at Savè supersite, in Benin. Our analysis, which starts since the stratiform cloud formation usually at night, focuses on the role played by the coupling between the cloud and the surface in the transition towards shallow convective clouds. It is based on several diagnostics, including Richardson number and various cloud macrophysical properties. The distance between lifting condensation level and cloud base height is used as a criterion of coupling. We also make an attempt to estimate the most predominant terms of the liquid water path budget on early morning. When the nocturnal low-level stratiform cloud forms, it is decoupled from the surface, except in one case. On early morning, the cloud is found coupled with the surface in nine cases and is remained decoupled in the thirteen other cases. The coupling, which occurs within the four hours after the cloud formation, is accompanied with a cloud base lowering and near-neutral thermal stability in the subcloud layer. Further, at the initial stage of the transition, the stratiform cloud base is slightly cooler, wetter and more homogeneous in the coupled cases. The moisture jump at cloud top is found usually around 2 g kg−1, and the temperature jump within 1–5 K, which is significantly smaller than typical marine stratocumulus, and explained by the monsoon flow environment within which the stratiform cloud develops. No significant difference of liquid water path budget terms was found between the coupled and decoupled cases. In agreement with previous numerical studies, we found that the stratiform cloud maintenance before the sunrise results from the interplay between the predominant radiative cooling, and, the entrainment and large scale subsidence at its top. Three transition scenarios were observed, depending on the state of the coupling at the initial stage. In the coupled cases, the low-level stratiform cloud remains coupled until its break up. In five of the decoupled cases, the cloud couples with the surface as the LCL is rising. In the eight remaining cases, the stratiform cloud remains decoupled from the surface all along its life cycle. In case of coupling during the transition, the stratiform cloud base lifts with the growing convective boundary layer roughly between 06:30 and 08:00 UTC. The cloud deck breakup occurring at 11:00 UTC or later leads to the formation of shallow convective clouds. When the decoupling subsists, shallow cumulus clouds form below the stratiform cloud deck between 06:30 and 09:00 UTC. The breakup time in this scenario has a stronger variability, and occurs before 11:00 UTC in most of the cases. Thus we argue that the coupling with the surface during the daytime hours has a crucial role in the low-level stratiform cloud maintenance and in its transition towards shallow convective clouds.