4.7 Article

Characterization of Submesoscale Turbulence in the East/Japan Sea Using Geostationary Ocean Color Satellite Images

期刊

GEOPHYSICAL RESEARCH LETTERS
卷 46, 期 14, 页码 8214-8223

出版社

AMER GEOPHYSICAL UNION
DOI: 10.1029/2019GL083892

关键词

submesoscale observation; geostationary satellite; chlorophyll a; kinetic energy spectra; velocity structure function; energy flux

资金

  1. Korean Research Fellowship (KRF) from the National Research Foundation (NRF) [2017H1D3A1A01013959]
  2. research project titled Technology development for practical applications of multi-satellite data to maritime issues - Ministry of Oceans and Fisheries [20180455]
  3. research project titled Investigation and prediction system development of marine heatwave around the Korean Peninsula originated from the subarctic and western Pacific - Ministry of Oceans and Fisheries [20190344]
  4. National Research Foundation of Korea [2017H1D3A1A01013959] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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Submesoscale processes are key in understanding physical and biological phenomena near the surface, but there remains a lack of observational evidence over large areas. We used hourly images from a geostationary satellite that can resolve variation in surface ocean color over an area of few hundred kilometers. The temporal variation in the surface chlorophyll a distribution captured by the satellite images was first used to generate a submesoscale-permitting velocity field, from which we calculated the turbulence statistics such as kinetic energy spectra, velocity structure functions, and energy flux. Application to the April scenes in the East/Japan Sea showed that the kinetic energy spectra had a transition scale at 50 km that suggested two spectral regimes following k(-3) and k(-5/3), implying the coexistence of quasi-geostrophic turbulence and surface quasi-geostrophic turbulence. The chlorophyll a scalar spectrum suggested two spectral regimes of k(-5/3) and k(-1) with a transition at 3 km.

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