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A model study of Luzon cold eddies in the northern South China Sea

机译:南海北部吕宋冷涡的模型研究

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摘要

A variable-grid global ocean circulation model (MITgcm) was employed to study the effects of wind and Kuroshio intrusion on the Luzon cold eddies (LCEs) in the northern South China Sea (SCS). Study findings showed that there are two cold eddies northwest of the Luzon Island. The cold eddies above 300 m and below 500 m depth are referred to as the upper and lower layer LCE, respectively, based on their different generation sites, properties and dynamic mechanisms in these layers. In this study, the upper layer LCE was mainly induced by the winter wind stress curl in the SCS and generated northwest of the Luzon Island in late November, but it may have been weakened by the Kuroshio intrusion. It moved northwestward and decayed at about (115 degrees E, 20 degrees N) in late June. The center of the upper layer LCE tilted westward with increasing depth until March. The vorticity intensity of the upper layer LCE peaked in December to January and generally decreased with depth. The contributions of both wind stress curl and Kuroshio intrusion to the generation of the lower layer LCE were roughly equal. The lower layer LCE originated from a cold eddy, which moved westward from the Luzon Strait in August through October and then intensified by wind stress curl. Subsequently, it moved westward with a slight southward migration and finally decayed near the Xisha Islands in April to May. Its amplitude and radius reached a maximum around December, while the vorticity intensity peaked in January to February. (C) 2015 Elsevier Ltd. All rights reserved.
机译:利用可变网格全球海洋环流模型(MITgcm)研究了风和黑潮入侵对南海北部(SCS)的吕宋冷涡(LCE)的影响。研究结果表明,吕宋岛西北部有两个冷涡。深度大于300 m和深度小于500 m的冷涡基于它们在这些层中的不同生成部位,性质和动力机制而分别称为上层和下层LCE。在这项研究中,上层LCE主要是由南海的冬季风应力卷曲引起的,并于11月下旬在吕宋岛的西北部产生,但可能由于黑潮的入侵而减弱了。它向西北移动,并于6月下旬在大约(东经115度,北纬20度)处衰减。上层LCE的中心随着深度的增加向西倾斜,直到三月。上层LCE的涡旋强度在12月至1月达到峰值,并随深度而总体下降。风应力卷曲和黑潮侵入对下层LCE产生的贡献大致相等。下层LCE源自冷涡,该涡在8月至10月从吕宋海峡向西移动,然后由于风应力卷曲而加剧。随后,它向西移动,并向南移动一点,最后在4月至5月在西沙群岛附近腐烂。其振幅和半径在12月左右达到最大值,而涡旋强度在1月至2月达到峰值。 (C)2015 Elsevier Ltd.保留所有权利。

著录项

  • 来源
    《Deep-Sea Research》 |2015年第3期|107-123|共17页
  • 作者单位

    Chinese Acad Sci, South China Sea Inst Oceanol, State Key Lab Trop Oceanog, Guangzhou 510301, Guangdong, Peoples R China;

    Chinese Acad Sci, South China Sea Inst Oceanol, State Key Lab Trop Oceanog, Guangzhou 510301, Guangdong, Peoples R China;

    Chinese Acad Sci, South China Sea Inst Oceanol, State Key Lab Trop Oceanog, Guangzhou 510301, Guangdong, Peoples R China;

    Chinese Acad Sci, South China Sea Inst Oceanol, State Key Lab Trop Oceanog, Guangzhou 510301, Guangdong, Peoples R China|Univ Chinese Acad Sci, Beijing 100049, Peoples R China;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Luzon cold eddy; Vertical structure; Eddy energy; Numerical model; South China Sea;

    机译:吕宋冷涡垂直结构涡能量数值模型南中国海;

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