Content area
The spatial and seasonal characteristics of submesoscales in the Northwest Pacific Subtropical Ocean are thoroughly investigated here using a submesoscale-permitting model within a localized multiscale energetics framework, in which three scale windows termed background, mesoscale, and submesoscale are decomposed. It is found that submesoscale energetics are highly geographically inhomogeneous. In the Luzon Strait, baroclinic and barotropic instabilities are the primary mechanisms for generating submesoscale available potential energy (APE) and kinetic energy (KE), and they exhibit no significant seasonal variations. Although buoyancy conversion experiences pronounced seasonal cycles and serves as the main sink of submesoscale APE in winter and spring, its contribution to submesoscale KE is negligible. The major sinks of submesoscale KE are advection, horizontal pressure work, and dissipation. In the Western Boundary Current transition and Subtropical Countercurrent (STCC) interior open ocean zone, submesoscales undergo significant seasonality, with large magnitudes in winter and spring. In spring and winter, baroclinic instability dominates the generation of submesoscale APE via forward cascades, while KE is mainly energized by buoyancy conversion and dissipated by the residual term. Meanwhile, in summer and autumn, submesoscales are considerably weak. Additionally, submesoscale energetics in the Western Boundary Current transition zone are slightly greater than those in the STCC interior open ocean zone, which is attributed to the strengthened straining of the Western Boundary Current and mesoscale eddies.
Details
Transition zone;
Eddies;
Seasonal variation;
Datasets;
Potential energy;
Buoyancy;
Baroclinic instability;
Topography;
Windows (computer programs);
Seasonal variations;
Mesoscale eddies;
Spring;
Simulation;
Spring (season);
Winter;
Mesoscale phenomena;
Dissipation;
Ocean circulation;
Seasonality;
Barotropic mode
; Zhang, Shaoqing 2
; Wang, Kaidi 3 ; Yu Yangyang 4 ; Gao, Yang 5
; Cui, Tong 6 1 College of Oceanic and Atmospheric Sciences, Ocean University of China, Qingdao 266100, China; [email protected], Frontiers Science Center for Deep Ocean Multispheres and Earth System (FDOMES), Key Laboratory of Physical Oceanography, Ministry of Education, Ocean University of China, Qingdao 266100, China
2 College of Oceanic and Atmospheric Sciences, Ocean University of China, Qingdao 266100, China; [email protected], Frontiers Science Center for Deep Ocean Multispheres and Earth System (FDOMES), Key Laboratory of Physical Oceanography, Ministry of Education, Ocean University of China, Qingdao 266100, China, Laboratory for Ocean Dynamics and Climate, Qingdao Marine Science and Technology Center, Qingdao 266100, China
3 Qingdao Institute of Marine Meteorology, Chinese Academy of Meteorological Sciences, Qingdao Research Center of Marine Meteorology, Qingdao 266404, China; [email protected]
4 The First Institute of Oceanography, Ministry of Natural Resources, Qingdao 266061, China; [email protected]
5 Frontiers Science Center for Deep Ocean Multispheres and Earth System (FDOMES), Key Laboratory of Marine Environmental Science and Ecology, Ministry of Education, Ocean University of China, Qingdao 266100, China; [email protected]
6 Qingdao Leice Transient Technology Co., Ltd., Qingdao 266100, China; [email protected]