2017
DOI: 10.1175/jpo-d-16-0185.1
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Anticyclonic Eddy Sheddings from Kuroshio Loop and the Accompanying Cyclonic Eddy in the Northeastern South China Sea

Abstract: Sheddings of Kuroshio Loop Current (KLC) eddies in the northeastern South China Sea (SCS) are investigated using mooring arrays, multiple satellite data, and data-assimilative HYCOM products. Based on altimeter sea surface heights between 1992 and 2014, a total of 19 prominent KLC eddy shedding (KLCES) events were identified, among which four events were confirmed by the concurrent moored and satellite observations. Compared to the leaping behavior of Kuroshio, KLCES is a relatively short-duration phenomenon t… Show more

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Cited by 128 publications
(175 citation statements)
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“…It should be noted that the seasonality of submesoscales in region ST (i.e., stronger in winter and weaker in summer) is essentially not determined by the state of the Kuroshio but by the total available potential energy stored in the mixed layer. Although the Kuroshio loop tends to occur in winter (not always) that can indeed strengthen the MSR in region ST, it is an unstable state and is usually terminated by eddy shedding (Nan et al, ; Zhang et al, ). A good example to demonstrate the indeterministic role of Kuroshio is that even after the Kuroshio eddy shedding (Kuroshio returns to its usual gap‐leaping state), the submesoscales are still very active in region ST in winter (Figure S5).…”
Section: Summary and Discussionmentioning
confidence: 99%
“…It should be noted that the seasonality of submesoscales in region ST (i.e., stronger in winter and weaker in summer) is essentially not determined by the state of the Kuroshio but by the total available potential energy stored in the mixed layer. Although the Kuroshio loop tends to occur in winter (not always) that can indeed strengthen the MSR in region ST, it is an unstable state and is usually terminated by eddy shedding (Nan et al, ; Zhang et al, ). A good example to demonstrate the indeterministic role of Kuroshio is that even after the Kuroshio eddy shedding (Kuroshio returns to its usual gap‐leaping state), the submesoscales are still very active in region ST in winter (Figure S5).…”
Section: Summary and Discussionmentioning
confidence: 99%
“…The unbalanced processes, such as submesoscale instabilities, strain‐induced frontogenesis, and internal waves, are responsible for the scale transition from balanced to unbalanced states traversing the mesoscale and submesoscale (Benthuysen & Thomas, ; Fox‐Kemper et al, ; Gula et al, ; McWilliams, ). In the NSCS, the KE spectrum is primarily composed of energetic vortex modes and wave components, which are representative of active eddy variability (Chavanne & Klein, ; Zhang et al, ) and internal waves (Alford et al, ; Tian et al, ). Based on the limited observations and high‐resolution model output, this paper preliminarily examines the wave‐vortex and rotational‐divergent KE spectra in the mesoscale and submesoscale ranges and provides an improved understanding of the strength of balanced versus unbalanced motions and the dominant wavelengths for the KE and SSH in the NSCS.…”
Section: Summary and Discussionmentioning
confidence: 99%
“…Owing to the debates on the intrusion paths, there is no clear definition of the KI. To clarify the KI phenomenon in this paper, an approach similar to that used by Chern et al (2010) is adopted, and the KI is defined as the Kuroshio Loop Current (red dotted path in Figure 1), which has been widely verified by both observations (Centurioni et al, 2004;Farris & Wimbush, 1996;Li & Wu, 1989;Zhang et al, 2017) and numerical simulations (Chern et al, 2010;Metzger & Hurlburt, 2001).…”
Section: Introductionmentioning
confidence: 89%
“…The analyses in the above section suggest that triggering of the KI is attributed to the eddy‐current interaction. To understand this interaction, the eddy‐energetic analysis (Tsujino et al, ), which has been used to study the eddy shedding process caused by the KI in Zhang et al (), is employed. The related equations are written as follows: BT=()ugvg()ugy+vgx+ugugugx+vgvgvgy, BC=g2ρ02N2()ugρρx+vgρρy, WSW=τwuu0+τwvv0ρ0. …”
Section: Oprs Triggering the Ki Occurrencementioning
confidence: 99%
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