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Dynamics of the Northern Tsuchiya Jet

机译:土屋北急流的动力学

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摘要

The Tsuchiya jets (TJs) are narrow eastward currents located along thermal fronts at the poleward edges of thermostad water in the Pacific Ocean. In this study, an oceanic general circulation model (OGCM) is used to explore the dynamics of the northern TJ. Solutions are found in a rectangular basin, extending 100° zonally and from 40°S to 40°N. They are forced by three idealized forcings: several patches of idealized wind fields, including one that simulates the strong Ekman pumping region in the vicinity of the Costa Rica Dome (CRD); surface heating that warms the ocean in the tropics; and a prescribed interocean circulation (IOC) that enters the basin through the southern boundary and exits through the western boundary from 2° to 6°N (the model's Indonesian passages).rnSolutions forced by all the aforementioned processes and with minimal diffusion resemble the observed flow field in the tropical North Pacific. A narrow eastward current, the model's northern TJ, flows across the basin along the northern edge of a thick equatorial thermostad. Part of the TJ water upwells at the CRD upwelling region and the rest returns westward in the lower part of the North Equatorial Current. The deeper part of the TJ is supplied by water that leaves the western boundary current somewhat north of the equator. Its shallower part originates from water that diverges from the deep portion of the Equatorial Undercurrent (EUC); as a result, the TJ transport increases to the east and the TJ warms as it flows across the basin. These and other properties suggest that the dynamics of the model's TJ are those of an arrested front, which in a 2%-layer model are generated when characteristics of the flow converge strongly or intersect.rnEddy form stress, due to instability waves generated at the CRD region, extends the TJ circulation to deeper levels. When diffusivity is increased to commonly used values, the thermostad is less well defined and the TJ is weak. In a solution without the IOC, the TJ is shifted to higher temperatures with its water supplied by the subtropical cell. When horizontal viscosity is reduced, the TJ becomes narrower and is flanked by a westward current on its equatorward side.
机译:Tsuchiya喷流(TJs)是狭窄的向东流,沿着太平洋上的热稳定水极向边缘的热锋位于热锋线上。在这项研究中,海洋大环流模型(OGCM)用于探索北部TJ的动力学。在矩形盆地中找到解决方案,该盆地在纬向延伸100°,从40°S延伸到40°N。它们受到三个理想化强迫的推动:几个理想化风场,其中一个模拟了哥斯达黎加巨蛋(CRD)附近的强力埃克曼抽水区;加热热带地区海洋的地表加热;并且规定的海洋环流(IOC)从南边界进入盆地并从西边界从2°N到6°N离开(模型的印尼通道)。热带北太平洋的流场。狭窄的东流,即该模型的北TJ,沿着厚赤道热区的北边缘流经盆地。 TJ水上升流的一部分在CRD上升区,其余则在北赤道洋流的下部向西回流。 TJ的较深部分由水供应,而水则离开西部边界流到赤道以北。它的较浅部分来自于从赤道暗流(EUC)的较深部分发散的水。结果,TJ运移向东部增加,并且TJ在流经盆地时变暖。这些和其他特性表明,模型TJ的动力学是滞留前沿的动力学,在流动为2%的层模型中,当流动的特性强烈收敛或相交时会生成该模型。 CRD区域将TJ循环扩展到更深的层次。当扩散率增加到常用值时,热稳定度的定义不太好,TJ较弱。在没有IOC的解决方案中,TJ的水由亚热带电池供应,从而转变为更高的温度。当水平粘度降低时,TJ变窄,并在赤道侧被向西流向两侧。

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  • 来源
    《Journal of Physical Oceanography》 |2009年第9期|2024-2051|共28页
  • 作者单位

    University of Hawaii at Manoa, POST BIdg., 4th Floor, 1680 East-West Rd., Honolulu, HI 96822;

    International Pacific Research Center, SOEST, University of Hawaii at Manoa, Honolulu, Hawaii;

    International Pacific Research Center, SOEST, University of Hawaii at Manoa, Honolulu, Hawaii;

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