期刊
JOURNAL OF THE ATMOSPHERIC SCIENCES
卷 80, 期 6, 页码 1547-1563出版社
AMER METEOROLOGICAL SOC
DOI: 10.1175/JAS-D-22-0184.1
关键词
Marine boundary layer; Cumulus clouds; Diabatic heating; Mixing; Stability; Buoyancy
Using observations from the EUREC4A campaign, a new conceptual picture of the trade wind transition layer is proposed. Cloud formation mainly occurs within the transition layer, and the cloud-top height distribution is bimodal. The life cycle of the first cloud population maintains the transition-layer structure through a condensation-evaporation mechanism.
The transition layer in the trades has long been observed and simulated, but the physical processes producing its structure remain little investigated. Using extensive observations from the Elucidating the Role of Clouds-Circulation Coupling in Climate (EUREC4A) field campaign, we propose a new conceptual picture of the trade wind transition layer, occurring between the mixed-layer top (around 550 m) and subcloud-layer top (around 700 m). The theory of cloud-free convective boundary layers suggests a transition-layer structure with strong jumps at the mixed-layer top, yet such strong jumps are only observed rarely. Despite cloud-base cloud fraction measured as only 5.3% 6 3.2%, the canonical cloud-free convective boundary layer structure is infrequent and confined to large [O(200) km] cloud-free areas. We show that the majority of cloud bases form within the transition layer, instead of above it, and that the cloud-top height distribution is bimodal, with a first population of very shallow clouds (tops below 1.3 km) and a second population of deeper clouds (extending to 2-3 km depth). We then show that the life cycle of this first cloud population maintains the transition-layer structure. That is, very shallow clouds smooth vertical thermodynamic gradients in the transition layer by a condensation- evaporation mechanism, which is fully coupled to the mixed layer. Inferences from mixed-layer theory and mixing diagrams, moreover, suggest that the observed transition-layer structure does not affect the rate of entrainment mixing, but rather the properties of the air incorporated into the mixed layer, primarily to enhance its rate of moistening.
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