A large-eddy simulation study of deep-convection initiation through the collision of two sea-breeze fronts

被引:24
作者
Fu, Shizuo [1 ,2 ]
Rotunno, Richard [3 ]
Chen, Jinghua [4 ,5 ]
Deng, Xin [6 ]
Xue, Huiwen [7 ]
机构
[1] Fujian Normal Univ, Key Lab Humid Subtrop Ecogeog Proc, Minist Educ, Fuzhou, Peoples R China
[2] Fujian Normal Univ, Sch Geog Sci, Fuzhou, Peoples R China
[3] Natl Ctr Atmospher Res, POB 3000, Boulder, CO 80307 USA
[4] Nanjing Univ Informat Sci & Technol, Collaborat Innovat Ctr Forecast & Evaluat Meteoro, China Meteorol Adm, Nanjing, Peoples R China
[5] Nanjing Univ Informat Sci & Technol, Key Lab Aerosol Cloud Precipitat, China Meteorol Adm, Nanjing, Peoples R China
[6] Fujian Agr & Forestry Univ, Coll Agr, Fuzhou, Fujian, Peoples R China
[7] Peking Univ, Sch Phys, Dept Atmospher & Ocean Sci, Beijing, Peoples R China
基金
中国国家自然科学基金; 美国国家科学基金会;
关键词
FINESCALE VERTICAL STRUCTURE; MOIST CONVECTION; AIRBORNE DOPPLER; STORM INITIATION; LAKE BREEZES; COLD-FRONT; JUNE; 2002; PART I; LAYER; BOUNDARIES;
D O I
10.5194/acp-21-9289-2021
中图分类号
X [环境科学、安全科学];
学科分类号
08 ; 0830 ;
摘要
Deep convection plays important roles in producing severe weather and regulating the large-scale circulation. However, deep-convection initiation (DCI), which determines when and where deep convection develops, has not yet been fully understood. Here, large-eddy simulations are performed to investigate the detailed processes of DCI, which occurs through the collision of two sea-breeze fronts developing over a peninsula. In the simulation with a maximum total heat flux over land of 700 or 500 W m(-2), DCI is accomplished through the development of three generations of convection. The first generation of convection is randomly produced along the colliding sea-breeze fronts. The second generation of convection only develops in regions where no strong downdrafts are produced by the first generation of convection and is also mainly produced through the collision of the sea-breeze fronts. The third generation of convection mainly develops from the intersection points of the cold pools produced by the second generation of convection and is produced through the collision between the gust fronts and the sea-breeze fronts. Decreasing the maximum total heat flux from 700 to 500 W m(-2) weakens each generation of convection. Further decreasing the maximum total heat flux to 300 W m(-2) leads to only one generation of shallow convection.
引用
收藏
页码:9289 / 9308
页数:20
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