4.7 Article

Submesoscale Eddy and Frontal Instabilities in the Kuroshio Interacting With a Cape South of Taiwan

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AMER GEOPHYSICAL UNION
DOI: 10.1029/2020JC016123

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  1. CWB of Taiwan [1062076C]
  2. Ministry of Science and Technology of Taiwan (MOST) [103-2611-M-002-018, 105-2611-M-002-012, 107-2611-M-002-015]
  3. MOST [101-2611-M-002-018-MY3, 103-2611-M-002-011, 105-2119-M-002-042]
  4. U.S. Office of Naval Research Grant [N000141613069]
  5. U.S. Department of Defense (DOD) [N000141613069] Funding Source: U.S. Department of Defense (DOD)

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The processes underlying the strong Kuroshio encountering a cape at the southernmost tip of Taiwan are examined with satellite-derived chlorophyll and temperature maps, a drifter trajectory, and realistic model simulations. The interaction spurs the formation of submesoscale cyclonic eddies that trap cold and high-chlorophyll water and the formation of frontal waves between the free stream and the wake flow. An observed train of eddies, which have relative vorticity about one to four times the planetary vorticity (f), is shed from the recirculation that occurs in the immediate lee of the cape as a result of flow separation. These propagate downstream at a speed of 0.5-0.6 m s(-1) . Farther downstream, the corotation and merging of two or three adjacent eddies are common owing to the topography-induced slowdown of eddy propagation farther downstream. It is found that the relative vorticity of a corotating system (1.2f) is 70% weaker than that of a single eddy due to the increase of eddy diameter from similar to 16 to similar to 33 km, in agreement with Kelvin's circulation theorem. The shedding period of the submesoscale eddies is strongly modulated by either diurnal or semidiurnal tidal flows, which typically reach 0.2-0.5 m s(-1) , whereas its intrinsic shedding period is insignificant. The frontal waves predominate in the horizontal free shear layer emitted from the cape, as well as a density front. Energetics analysis suggests that the wavy features result primarily from the growth of harotropic instability in the free shear layer, which may play a secondary process in the headland wake.

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