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Circling in on Convective Self‐Aggregation

In radiative‐convective equilibrium simulations, convective self‐aggregation (CSA) is the spontaneous organization into segregated cloudy and cloud‐free regions. Evidence exists for how CSA is stabilized, but how it arises favorably on large domains is not settled. Using large‐eddy simulations, we l...

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Detalles Bibliográficos
Autores principales: Nissen, Silas Boye, Haerter, Jan O.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9285845/
https://www.ncbi.nlm.nih.gov/pubmed/35864905
http://dx.doi.org/10.1029/2021JD035331
Descripción
Sumario:In radiative‐convective equilibrium simulations, convective self‐aggregation (CSA) is the spontaneous organization into segregated cloudy and cloud‐free regions. Evidence exists for how CSA is stabilized, but how it arises favorably on large domains is not settled. Using large‐eddy simulations, we link the spatial organization emerging from the interaction of cold pools (CPs) to CSA. We systematically weaken simulated rain evaporation to reduce maximal CP radii, [Formula: see text] , and find reducing [Formula: see text] causes CSA to occur earlier. We further identify a typical rain cell generation time and a minimum radius, [Formula: see text] , around a given rain cell, within which the formation of subsequent rain cells is suppressed. Incorporating [Formula: see text] and [Formula: see text] , we propose a toy model that captures how CSA arises earlier on large domains: when two CPs of radii [Formula: see text] collide, they form a new convective event. These findings imply that interactions between CPs may explain the initial stages of CSA.