Influence of typhoon “MITAG” on the Kuroshio intrusion in the Luzon Strait during early fall 2019
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Abstract: Typhoons in the Western Pacific have a significant impact on the transport of heat, salt and particles through the Luzon Strait. However, there are very limited field observations of this impact because of extreme difficulties and even dangers for ship-based measurements during the rough weather. Here, we present the preliminary results from analyzing a dataset collected by a glider deployed west of the Luzon Strait a few days prior to the arrival of typhoon “MITAG”. The gilder data revealed an abnormally salinity (>34.8) subsurface water apparently sourced from Kuroshio intrusion during the typhoon. When typhoon “MITAG” traveled on the east of the Luzon Strait, the positive wind stress curl strengthened the cyclonic eddy and weakened the anti-cyclonic eddy. This led to a slowdown of Kuroshio and made its intrusion easier. The main axis of the Kuroshio at the northern part of the strait shifted westward after the typhoon and did not return to its original position until a week later. The Ekman transport from persistent northerly wind of typhoon “MITAG” was significant, but its importance in enhancing the Kuroshio intrusion is only secondary relative to the eddies variations.
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Key words:
- typhoon /
- glider /
- Kuroshio intrusion /
- Luzon Strait
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Figure 3. The time series vertical distribution of potential temperature (a), salinity (b), potential density (c), and calculated buoyancy frequency (d). The latitudes at which the gilder was located on certain days were also marked. The white solid lines denote the MLD, the magenta dashed line indicate that the change in direction of glider, the white and black dashed lines indicate the period of passing east of LS for typhoon “MITAG” (Fig. 1), and the blue dashed lines in (b) suggest the boundaries of the high salinity water mass (>34.8).
Figure 4. The time series vertical distribution of potential temperature anomaly (a), salinity anomaly (b), potential density anomaly (c), and mean vertical temperature (d). The latitudes at which the gilder was located on certain days were also marked. The white solid lines denote the MLD, the magenta dashed line indicate that the change in direction of glider, the white and black dashed lines indicate the period of passing east of LS for typhoon “MITAG” (Fig. 1), and the blue dashed lines in b suggest the boundaries of the high salinity water mass (>34.8).
Figure 5. T-S diagrams of CS1/2 and Argo profiles (a) and the climatology salinity maximum at a depth of 0–400 m for September (b) and October (c), respectively. In a, the blue thick line represents the averaged T-S curves for the northeastern SCS water (SCSW), and the red thick line represents Kuroshio water (KW), based on WOA 18 climatology data. The rectangles in b indicate the sampling location of different water masses: the northeastern SCS Water (SCSW, 18°–22°N, 116°–120.5°E) is marked in blue, and the Kuroshio water (KW, 18°–22°N, 122°–124°E) is indicated in red. The cyan dots in c are glider paths, and the magenta dots are locations of Argo floats.
Figure 7. Time evolution of the SLA (m) and geostrophic currents (m/s) from September 28 to October 14, 2019. Regions shallower than 200 m are masked. The observed section is represented by cyan dots. The positions of the glider during that day are denoted by red dots. The yellow and magenta dots are the trajectories of Typhoon and Argo float, respectively. The green rectangular frame is used to show the axis of the Kuroshio current, and the blue boxes is area in which the variations of total relative vorticity and EPV are calculated. The cyclonic and anti-cyclonic eddies in the blue box are denoted as “CE” and “AE”.
Figure 8. Variations of the Kuroshio current during the study period, represented by the geostrophic current meridional velocity (m/s). (a) The movement of the Kuroshio current axis from 120.125°E to 121.875°E. The contour map indicates the northward meridional vector of the Kuroshio current. Each grid represents a velocity maximum and their longitude in the green rectangular (20.125°–21.875°N, 120.125°–121.875°E) in Fig. 7a. The black dots are the position of the Kuroshio current main axis. (b) The velocity variation of the Kuroshio current main axis near 21°N. (c) The velocity variation of the Kuroshio current main axis near 18.5°N. (d) The variation of total relative vorticity in the CE (blue line) and AE (red line) and EPV (orange and green lines) in the blue box (18°–22°N, 122°–124°E) in Fig. 7. The orange line indicate the total EPV calculated in the box (18°–22°N, 122°–124°E), and green line indicate the total EPV calculated in the box (18°N–20°N, 122°E–124°E). The positive value of EPV indicate the Ekman upwelling. (e) The variation of SLA in the center of CE (blue line) and AE (orange line).
Figure 9. Distribution of wind field, wind stress curl (a, b, c) and Ekman transport (d, e, f) when the typhoon passed east of the Luzon Strait. The contour maps in a, b, and c display the wind curl, and the arrows indicate the wind velocity and direction. The contour maps in d, e, and f show the Ekman transport per unit width, and the arrows represent directions.
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