日本以南海域中尺度涡统计特征与三维结构

Statistical Characteristics and Three-Dimensional Structures of Mesoscale Eddies in the Sea South of Japan

  • 摘要: 基于META3.2 DT涡旋轨迹数据和ARMOR3D温盐流数据,本研究系统分析了1993—2021年日本以南海域(131°~142°E, 28°~35°N)半径超过50 km的中尺度涡的统计特征与三维结构。结果表明,研究区域内每日气旋涡与反气旋涡的平均数量分别为3.6和2.8个;约75%的气旋涡半径介于50~110 km、振幅介于0~25 cm;约75%的反气旋涡半径介于50~130 km、振幅介于0~20 cm;约75%的气旋涡和反气旋涡生命周期在40 d以内。研究区域南部的开阔大洋中,气旋涡与反气旋涡均主要向西传播;黑潮及其北侧海域,大多数气旋涡向东传播,而其南侧海域,部分反气旋涡也向东传播。气旋涡频发于黑潮北侧以(137°30′E, 33°30′N)为中心的海域,这主要由正压不稳定、斜压不稳定和黑潮正涡度输入所致。反气旋涡则频发于黑潮南侧以(136°00′E, 31°30′N)为中心的海域,这主要由斜压不稳定和黑潮负涡度输入所引起。在垂直方向上,气旋涡影响深度超过1 200 m,而反气旋涡影响深度约为1 000 m。气旋涡和反气旋涡均表现出次表层加强型特征,二者引起的最大温度与盐度异常均出现在约400 m深度层。此外,气旋涡和反气旋涡均无明显倾斜。本研究深化了对日本以南海域中尺度涡统计特征与三维结构的认知,为进一步探究涡旋与黑潮的相互作用等奠定了基础,为我国在相关海域航行安全保障及海洋环境预报等提供了科学参考。

     

    Abstract: Based on the META3.2 DT mesoscale eddy trajectory data and the ARMOR3D temperature, salinity, and current data, the statistical characteristics and three-dimensional structures of cyclonic and anticyclonic eddies with radii exceeding 50 km in the sea south of Japan (131°-142°E, 28°-35°N, the study region) during 1993-2021 were systematically analyzed. The results show that the mean daily numbers of cyclonic and anticyclonic eddies in the study region are 3.6 and 2.8, respectively. Approximately 75% of cyclonic eddies have radii between 50 and 110 km and amplitudes ranging from 0 to 25 cm, while about 75% of anticyclonic eddies have radii between 50 and 130 km and amplitudes between 0 and 20 cm. Around 75% of both cyclonic and anticyclonic eddies have lifetimes shorter than 40 days. In the open ocean of the southern part of the study region, both cyclonic and anticyclonic eddies predominantly propagate westward. In contrast, within the Kuroshio and its northern flank, most cyclonic eddies propagate eastward, while within the southern flank of the Kuroshio, some anticyclonic eddies also exhibit eastward propagation. Cyclonic eddies frequently occur in the northern flank of the Kuroshio in the area centered at 137°30′E and 33°30′N. This is mainly attributed to barotropic instability, baroclinic instability, and the input of positive vorticity from the Kuroshio. Meanwhile, anticyclonic eddies frequently appear in the southern flank of the Kuroshio in the area centered at 136°00′E and 31°30′N. This is primarily caused by baroclinic instability and the input of negative vorticity from the Kuroshio. Vertically, the influence of cyclonic eddies penetrates over 1,200 m, whereas that of anticyclonic eddies is approximately 1 000 m. Both types of eddies exhibit subsurface-intensified structures, with the maximum temperature and salinity anomalies induced appearing at a depth of about 400 m. In addition, neither cyclonic nor anticyclonic eddies show obvious vertical tilting. This study enhances our understanding of the statistical characteristics and three-dimensional structures of mesoscale eddies in the sea south of Japan, providing a solid foundation for further investigations into eddy–Kuroshio interactions. It also serves as a scientific reference for China’s navigational safety and marine environment forecasting in relevant maritime regions.

     

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