Atmospheric Boundary Layer Structure and Turbulence during Sea Fog on the Southern China Coast

Huijun Huang Guangdong Provincial Key Laboratory of Regional Numerical Weather Prediction, and Joint Open Laboratory of Marine Meteorology, Institute of Tropical and Marine Meteorology, China Meteorological Administration, Guangzhou, China

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Hongnian Liu School of Atmospheric Sciences, Nanjing University, Nanjing, China

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Jian Huang Guangdong Provincial Key Laboratory of Regional Numerical Weather Prediction, and Joint Open Laboratory of Marine Meteorology, Institute of Tropical and Marine Meteorology, China Meteorological Administration, Guangzhou, China

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Weikang Mao Guangdong Provincial Key Laboratory of Regional Numerical Weather Prediction, and Joint Open Laboratory of Marine Meteorology, Institute of Tropical and Marine Meteorology, China Meteorological Administration, Guangzhou, China

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Xueyan Bi Guangdong Provincial Key Laboratory of Regional Numerical Weather Prediction, and Joint Open Laboratory of Marine Meteorology, Institute of Tropical and Marine Meteorology, China Meteorological Administration, Guangzhou, China

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Abstract

Small-scale turbulence has an essential role in sea-fog formation and evolution, but is not completely understood. This study analyzes measurements of the small-scale turbulence, together with the boundary layer structure and the synoptic and mesoscale conditions over the life cycle of a cold advection fog event and a warm advection fog event, both off the coast of southern China. The measurement data come from two sites: one on the coast and one at sea. These findings include the following: 1) For cold advection fog, the top can extend above the inversion base, but formation of an overlaying cloud causes the fog to dissipate. 2) For warm advection fog, two layers of low cloud can merge to form deep fog, with the depth exceeding 1000 m, when strong advection of warm moist air produces active thermal-turbulence mixing above the thermal-turbulence interface. 3) Turbulence near the sea surface is mainly thermally driven for cold advection fog, but mechanically driven for warm advection fog. 4) The momentum fluxes of both fog cases are below 0.04 kg m−1 s−2. However, the sensible and latent heat flux differ between the cases: in the cold advection fog case, the sensible and latent heat fluxes are roughly upward, averaging 2.58 and 26.75 W m−2, respectively; however, in the warm advection fog case, the sensible and latent heat flux are mostly downward, averaging −6.98 and −6.22 W m−2, respectively. 5) Low-level vertical advection is important for both fogs, but has a larger influence on fog development in the warm advection fog case.

Corresponding author address: Hongnian Liu, School of Atmospheric Sciences, Nanjing University, No. 22 Hankou Road, Nanjing, Jiangsu, 210093, China. E-mail: liuhn@nju.edu.cn

Abstract

Small-scale turbulence has an essential role in sea-fog formation and evolution, but is not completely understood. This study analyzes measurements of the small-scale turbulence, together with the boundary layer structure and the synoptic and mesoscale conditions over the life cycle of a cold advection fog event and a warm advection fog event, both off the coast of southern China. The measurement data come from two sites: one on the coast and one at sea. These findings include the following: 1) For cold advection fog, the top can extend above the inversion base, but formation of an overlaying cloud causes the fog to dissipate. 2) For warm advection fog, two layers of low cloud can merge to form deep fog, with the depth exceeding 1000 m, when strong advection of warm moist air produces active thermal-turbulence mixing above the thermal-turbulence interface. 3) Turbulence near the sea surface is mainly thermally driven for cold advection fog, but mechanically driven for warm advection fog. 4) The momentum fluxes of both fog cases are below 0.04 kg m−1 s−2. However, the sensible and latent heat flux differ between the cases: in the cold advection fog case, the sensible and latent heat fluxes are roughly upward, averaging 2.58 and 26.75 W m−2, respectively; however, in the warm advection fog case, the sensible and latent heat flux are mostly downward, averaging −6.98 and −6.22 W m−2, respectively. 5) Low-level vertical advection is important for both fogs, but has a larger influence on fog development in the warm advection fog case.

Corresponding author address: Hongnian Liu, School of Atmospheric Sciences, Nanjing University, No. 22 Hankou Road, Nanjing, Jiangsu, 210093, China. E-mail: liuhn@nju.edu.cn
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