Diagnostic calculation of the upper-layer circulation in the South China Sea during the winter of 1998

On the basis of hydrographic data obtained in November 28 to December 27, 1998 cruise, the calculation of the circulation in the South China Sea (SCS) is made by using the P-vector method, in combination with SSH data from TOPEX/ERS-2 analysis. For study of the dynamical mechanism, which causes the pattern of winter circulation in the SCS, the diagnostic model (Yuan et al., 1982; Yuan and Su, 1992) is used to simulate numerically the winter circulation in the SCS. The following results have been obtained. (1) The main characteristics of the circulation systems in the central SCS are as follows: A coastal southward jet in winter is present at the western boundary near the coast of Vietnam; there is a stronger cyclonic circulation with a larger horizontal scale east of this coastal southward jet and west of 114°E; there is a weaker anti-cyclonic circulation in the central part of eastern SCS; there is a stronger and northeastward flow opposing the northeasterly monsoon between above a stronger cyclonic circulation and a weaker anti-cyclonic circulation. (2) The circulation systems in the northern SCS are as follows: 1) There is a cyclonic circulation system northwest of Luzon, and it has three centers of the cold water; 2) There is an anti-cyclonic eddy. Its center is located near(20°N, 116°40' E); 3)There is a warm and anti-cyclonic circulation south of Hainan Island; 4) There is a northeastward flow, the South China Sea Warm Current, in winter off Guangdong coast in the northern SCS. (3) In the southern SCS there is an anti-cyclonic circulation, and also there is a smaller scale cold water and cyclonic eddy. (4) The above pattern of winter circulation in the SCS agrees qualitatively with the horizontal distribution of temperature at 200 m level. (5) The dynamical mechanism which produces the above basic pattern of winter circulation is because of the following two causes: 1) The joint effect of the baroclinity and relief (JEBAR) is an essential dynamical cause; 2) The interaction between the wind stress and bottom topographic (IBWT) under the strong northeasterly monsoon is the next important dynamical mechanism. (6) Comparing the hydrographic structure and the horizontal distribution of velocity with the SSH data from TOPEX/ERS-2 analysis in the SCS during December of 1998, it is found that they agree qualitatively.

南海海流对冬季风风应力的响应特征

本文用美国普林斯顿大学海洋模式（ＰＯＭ）的南海版本（ＳＣＳ－ＰＯＭ） 模拟了持续冬季风风应力作用下，南海海流的响应特征。结果表明，从静止的海洋 出发，定常冬季风风应力驱动下的南海海流有明显的时间变化，垂直积分后的海流 （全流）约需１２０天左右的时间，方能达到准稳定态，表层、次表层和深层海流的时 间演变也有类似特征。模拟结果还表明，ＳＣＳ－ＰＯＭ有能力模拟出南海边界流、沿 岸流和海流的涡旋状结构。

冬季寒潮期间黄、渤海水位低频波动研究

利用POM(Princeton Ocean Model)海洋数值模式建立渤、黄、东海冬季三维环流动力学区域模型。模型在海-气边界使用包括风应力、气压和热通量的大气驱动,海洋边界使用西太平洋模式提供的环流和潮位驱动,综合模拟潮波运动、温度、盐度、环流变化和水位低频波动。模拟了2001年1月寒潮过境时黄、渤海水位低频波动及流场变化,分析了其对大风过程、气压、降温的响应,发现冬季强劲的北风和西北风都可以通过抽吸振荡在渤、黄海诱发水位的低频波动,东北风则由于地形影响不能诱发渤、黄海的低频波动。气压和降温只是在波动幅度上有一定的影响。波动发源于渤海和北黄海,最大波幅可以达到0.6m。波动进入南黄海后有沿黄海深槽西侧传播的倾向,波动幅度在传播过程中逐渐减小。