Abstract:Mesoscale eddies are common in the ocean and their surface characteristics have been well revealed based on altimetric observations. Comparatively, the knowledge of the three-dimensional (3D) structure of mesoscale eddies is scarce, especially in the open ocean. In the present study, high-resolution field observations of a cyclonic eddy in the Kuroshio Extension have been carried out and the anatomy of the observed eddy is conducted. The temperature anomaly exhibits a vertical monopole cone structure with a ma… Show more
“…A cyclonic eddy field observation experiment was conducted over the area (156°E–160°E, 30.33°N–32°N) from June 26 to 30, 2014, with a total cruising distance of approximately 1,674 km (Figure 2) (Zhang et al., 2019). Zhang et al.…”
Section: Methodsmentioning
confidence: 99%
“…Zhang et al. (2019) established a field experiment with six zonal routes from south to north. The route closest to the eddy center (marked with a magenta square) is named S3.…”
Section: Methodsmentioning
confidence: 99%
“…The cyan line is the −0.1 m contour of surface level anomalies, which indicates the boundary of the cyclonic eddie (CE) in Zhang et al. (2019), and the black line is the 0.4 m/s contour of geostrophic velocity. The magenta square is the geometric center of the CE defined in the META 2.0 product (https://www.aviso.altimetry.fr/en/data/products/value-added-products/global-mesoscale-eddy-trajectory-product.html), which is closest to the survey line marked as S3.…”
Section: Methodsmentioning
confidence: 99%
“…The data collected in the layer of 5-1,000 m are used here. We refer the reader to Zhang et al (2019) for further information about this experiment.…”
Section: Field Datamentioning
confidence: 99%
“…A cyclonic eddy field observation experiment was conducted over the area (156°E-160°E, 30.33°N-32°N) from June 26 to 30, 2014, with a total cruising distance of approximately 1,674 km (Figure 2) (Zhang et al, 2019). Zhang et al (2019) established a field experiment with six zonal routes from south to north. The route closest to the eddy 2019), and the black line is the 0.4 m/s contour of geostrophic velocity.…”
Mesoscale eddies are ubiquitous in the world's oceans. They are rotated with a 10-100 km length scale. The relatively isolated water mass trapped with mesoscale eddies can propagate a long distance while maintaining the source thermohaline characteristics. Thus, there are significant differences in the thermohaline structures between the inside and outside eddies, which have profound effects on underwater acoustic propagation.The earliest studies on the impact of eddies on sound propagation were conducted by Vastano and Owens (1973) and Weinberg and Zabalgogeazcoa (1977) based on hydrological field data measured from a cyclonic Gulf Stream (GS) ring detected in 1967. Vastano and Owens (1973) first observed the significant acoustic field perturbation caused by the cyclonic ring in the relatively uniform acoustic environment of the Sargasso Sea and found a strong dispersion phenomenon of the ray path in the area where the sound channel depth changed with the ray computations. In the following year, Gemmill studied the eddy's effects on the convergence mode of sound propagation and revealed that the cold eddy destroys the cyclic distribution of the convergence zones and refracts the sound rays into the deep sound channel. Subsequently, the eddy effects on ray travel time, which reflects the sound arrival structure, were studied with a range-dependent model presented by Weinberg and Zabalgogeazcoa (1977). Although the above studies are valuable, the corresponding sensitivity investigations of sound propagation on the eddy property variation cannot be conducted because of the rarity of eddy field data. To address this problem, Henrick et al. (1977) established a parametric eddy model qualitatively validated by GS ring observation data. Through the model, the effects of eddy intensity, geometric size and peak rotation speed on sound transmission are studied. Due to the good performance of such a model in describing eddy sound
“…A cyclonic eddy field observation experiment was conducted over the area (156°E–160°E, 30.33°N–32°N) from June 26 to 30, 2014, with a total cruising distance of approximately 1,674 km (Figure 2) (Zhang et al., 2019). Zhang et al.…”
Section: Methodsmentioning
confidence: 99%
“…Zhang et al. (2019) established a field experiment with six zonal routes from south to north. The route closest to the eddy center (marked with a magenta square) is named S3.…”
Section: Methodsmentioning
confidence: 99%
“…The cyan line is the −0.1 m contour of surface level anomalies, which indicates the boundary of the cyclonic eddie (CE) in Zhang et al. (2019), and the black line is the 0.4 m/s contour of geostrophic velocity. The magenta square is the geometric center of the CE defined in the META 2.0 product (https://www.aviso.altimetry.fr/en/data/products/value-added-products/global-mesoscale-eddy-trajectory-product.html), which is closest to the survey line marked as S3.…”
Section: Methodsmentioning
confidence: 99%
“…The data collected in the layer of 5-1,000 m are used here. We refer the reader to Zhang et al (2019) for further information about this experiment.…”
Section: Field Datamentioning
confidence: 99%
“…A cyclonic eddy field observation experiment was conducted over the area (156°E-160°E, 30.33°N-32°N) from June 26 to 30, 2014, with a total cruising distance of approximately 1,674 km (Figure 2) (Zhang et al, 2019). Zhang et al (2019) established a field experiment with six zonal routes from south to north. The route closest to the eddy 2019), and the black line is the 0.4 m/s contour of geostrophic velocity.…”
Mesoscale eddies are ubiquitous in the world's oceans. They are rotated with a 10-100 km length scale. The relatively isolated water mass trapped with mesoscale eddies can propagate a long distance while maintaining the source thermohaline characteristics. Thus, there are significant differences in the thermohaline structures between the inside and outside eddies, which have profound effects on underwater acoustic propagation.The earliest studies on the impact of eddies on sound propagation were conducted by Vastano and Owens (1973) and Weinberg and Zabalgogeazcoa (1977) based on hydrological field data measured from a cyclonic Gulf Stream (GS) ring detected in 1967. Vastano and Owens (1973) first observed the significant acoustic field perturbation caused by the cyclonic ring in the relatively uniform acoustic environment of the Sargasso Sea and found a strong dispersion phenomenon of the ray path in the area where the sound channel depth changed with the ray computations. In the following year, Gemmill studied the eddy's effects on the convergence mode of sound propagation and revealed that the cold eddy destroys the cyclic distribution of the convergence zones and refracts the sound rays into the deep sound channel. Subsequently, the eddy effects on ray travel time, which reflects the sound arrival structure, were studied with a range-dependent model presented by Weinberg and Zabalgogeazcoa (1977). Although the above studies are valuable, the corresponding sensitivity investigations of sound propagation on the eddy property variation cannot be conducted because of the rarity of eddy field data. To address this problem, Henrick et al. (1977) established a parametric eddy model qualitatively validated by GS ring observation data. Through the model, the effects of eddy intensity, geometric size and peak rotation speed on sound transmission are studied. Due to the good performance of such a model in describing eddy sound
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