苏禄—苏拉威西海内孤立波动力参数时空变化特征
谢皆烁(1984—), 男, 安徽省宿州市人, 副研究员, 博士, 从事海洋内孤立波研究。email: |
Copy editor: 林强
收稿日期: 2021-12-24
修回日期: 2022-03-17
网络出版日期: 2022-04-19
基金资助
国家自然科学基金项目(42130404)
国家自然科学基金项目(41776008)
中国科学院前沿科学重点研究计划(QYZDJ-SSW-DQC034)
南方海洋科学与工程广东省实验室(广州)专项(GML2019ZD0304)
广东省自然资源厅专项([2020]017)
广东特支计划科技创新青年拔尖人才项目(2019TQ05H519)
广东省自然科学基金-面上项目(2020A1515010495)
广东省自然科学基金-面上项目(2021A1515012538)
广东省自然科学基金-面上项目(2021A1515011613)
Spatial-temporal variations of the dynamic parameters of internal solitary waves in the Sulu-Celebes Sea
Copy editor: LIN Qiang
Received date: 2021-12-24
Revised date: 2022-03-17
Online published: 2022-04-19
Supported by
Project of National Natural Science Foundation of China(42130404)
Project of National Natural Science Foundation of China(41776008)
Key Research Program of Frontier Sciences, CAS(QYZDJ-SSW-DQC034)
Southern Marine Science and Engineering Guangdong Laboratory (Guangzhou)(GML2019ZD0304)
Special project by Department of natural resources of Guangdong Province([2020]017)
Youth Science and Technology Innovation Talent of Guangdong TeZhi Plan(2019TQ05H519)
Natural Science Foundation of Guangdong Province(2020A1515010495)
Natural Science Foundation of Guangdong Province(2021A1515012538)
Natural Science Foundation of Guangdong Province(2021A1515011613)
基于弱非线性理论及再分析同化数据, 计算了苏禄—苏拉威西海冬季及夏季内孤立波动力参数, 包括内孤立波线性速度、一阶和二阶非线性参数及线性色散参数, 并研究了这些参数的时空变化特征。我们发现, 虽然苏拉威西海域受到更加显著的西北太平洋水入侵, 但苏禄海内孤立波动力参数的时空变化特征却比苏拉威西海更为显著。夏季苏禄海内孤立波线性速度总体上比冬季约大0.1m·s-1; 与此相反, 夏季苏拉威西海内孤立波线性速度却比冬季约小0.05m·s-1。无论是一阶或二阶非线性动力参数, 其在苏拉威西海的时空变化均比较微弱, 但在苏禄海则较为显著。苏禄海夏季一阶非线性动力参数比冬季高出约3×10-3s-1, 但是夏季二阶非线性动力参数却比1月份低约3×10-5m-1·s-1。此外, 相比冬季, 夏季苏禄海和苏拉威西海的色散动力参数均有所减弱, 但其在苏禄海减弱的幅度更大。综上, 苏禄—苏拉威西海环流引起的水体层化最大浮力频率所在深度的时空变化是造成上述内孤立波动力参数时空变化的根本原因。
谢皆烁 , 龚延昆 , 牛建伟 , 何映晖 , 陈植武 , 许洁馨 , 蔡树群 . 苏禄—苏拉威西海内孤立波动力参数时空变化特征[J]. 热带海洋学报, 2022 , 41(6) : 132 -142 . DOI: 10.11978/2021183
On the basis of the weakly nonlinear theory of internal solitary waves (ISWs) and the reanalyzed assimilation data in the Sulu-Celebes Sea in both summer and winter, we calculate the dynamic parameters of the ISWs, including the linear wave speed, the first- and second-order nonlinear parameters and the linear dispersion parameter, and investigate the spatial-temporal variations of these parameters. We find that, although the intrusion from the north Pacific Ocean into the Celebes Sea is very obvious, the spatial-temporal variations of the dynamic parameters of the ISWs in the Sulu Sea is more significant than that in the Celebes Sea. In the Sulu sea, the linear speed of ISW in summer is ~0.1 m·s-1 larger than that in winter; however, in the Celebes Sea, the linear speed of ISW in summer is ~0.05 m·s-1 smaller than that in winter. Regardless of the first- and second-order nonlinear parameters, their variations in the Celebes Sea are relatively weak, but in the Sulu Sea, their variations are significant. In the Sulu Sea, the first-order nonlinear parameter in summer is ~3×10-3 s-1 higher than that in winter, but the second-order nonlinear parameter in summer is ~3×10-5 m-1·s-1 lower than that in winter. In addition, in both the Sulu and Celebes Sea, the linear dispersion parameter in summer tends to reduce, but the reduction magnitude in Sulu Sea is relatively large. This paper shows that the variation in the depth of the maximum buoyancy frequency in the Sulu-Celebes Sea is the dominant factor that in turn results in the associated spatial-temporal variations of the dynamic parameters of ISWs.
图5 苏禄—苏拉威西海内孤立波线性速度c分布a. 1月; b. 8月。审图号为GS(2016)1609 Fig. 5 Linear speed of internal solitary waves in the Sulu-Celebes Sea |
图6 苏禄—苏拉威西海内孤立波一阶非线性参数α分布a. 1月; b. 8月。审图号为GS(2016)1609 Fig. 6 First-order nonlinear parameter α of internal solitary waves in the Sulu-Celebes Sea |
图7 苏禄—苏拉威西海内孤立波色散参数β分布a. 1月; b. 8月。审图号为GS(2016)1609 Fig. 7 Linear dispersion parameter β of internal solitary waves in the Sulu-Celebes Sea |
图8 苏禄—苏拉威西海内孤立波二阶非线性参数α1分布a. 1月; b. 8月。审图号为GS(2016)1609 Fig. 8 Second-order nonlinear parameter α1 of internal solitary waves in the Sulu-Celebes Sea |
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