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The TKE dissipation rate in the northern South China Sea
Authors:Iossif Lozovatsky  Zhiyu Liu  Harindra Joseph S Fernando  Jianyu Hu  Hao Wei
Institution:1. Environmental Fluid Dynamics Laboratories, Department of Civil & Environmental Engineering and Earth Sciences, University of Notre Dame, Notre Dame, IN, 46556, USA
2. State Key Laboratory of Marine Environmental Science, and Department of Physical Oceanography, College of Ocean & Earth Sciences, Xiamen University, 422 Siming South Road, Xiamen, 361005, China
4. Room C3-416 Xiping Building, Xiangan Campus, Xiamen University, Xiamen, 361102, China
3. College of Marine Science and Engineering, Tianjin University of Science & Technology, Tianjin, 300457, China
Abstract:The microstructure measurements taken during the summer seasons of 2009 and 2010 in the northern South China Sea (between 18°N and 22.5°N, and from the Luzon Strait to the eastern shelf of China) were used to estimate the averaged dissipation rate in the upper pycnocline 〈ε p〉 of the deep basin and on the shelf. Linear correlation between 〈ε p〉 and the estimates of available potential energy of internal waves, which was found for this data set, indicates an impact of energetic internal waves on spatial structure and temporal variability of 〈ε p〉. On the shelf stations, the bottom boundary layer depth-integrated dissipation $ {\widehat{\varepsilon}}_{\mathrm{BBL}} $ reaches 17–19 mW/m2, dominating the dissipation in the water column below the surface layer. In the pycnocline, the integrated dissipation $ {\widehat{\varepsilon}}_{\mathrm{p}} $ was mostly ~10–30 % of $ {\widehat{\varepsilon}}_{\mathrm{BBL}} $ . A weak dependence of bin-averaged dissipation $ \overline{\varepsilon} $ on the Richardson number was noted, according to $ \overline{\varepsilon}={\varepsilon}_0+\frac{\varepsilon_{\mathrm{m}}}{{\left(1+ Ri/R{i}_{\mathrm{cr}}\right)}^{1/2}} $ , where ε 0 + ε m is the background value of $ \overline{\varepsilon} $ for weak stratification and Ri cr?=?0.25, pointing to the combined effects of shear instability of small-scale motions and the influence of larger-scale low frequency internal waves. The latter broadly agrees with the MacKinnon–Gregg scaling for internal-wave-induced turbulence dissipation.
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