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首页> 外文期刊>Journal of Physical Oceanography >Coastal Wind-Driven Circulation in the Vicinity of a Bank. Part Ⅰ: Modeling Flow over Idealized Symmetric Banks
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Coastal Wind-Driven Circulation in the Vicinity of a Bank. Part Ⅰ: Modeling Flow over Idealized Symmetric Banks

机译:银行附近的沿海风驱动环流。第一部分:理想对称银行的建模流程

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摘要

This study examines how coastal banks influence wind-driven circulation along stratified continental shelves. Numerical experiments are conducted for idealized symmetric banks; the standard bank (200 km long and 50 km wide) has dimensions similar to the Heceta Bank complex along the Oregon shelf. Model runs are forced with 10 days of steady winds (0.1 Pa); upwelling and downwelling cases are compared. The bank introduces significant alongshelf variability in the currents and density fields. Upwelling-favorable winds create an upwelling front and a baroclinic jet (flowing opposite coastal-trapped wave propagation) that bend around the standard bank, approximately centered on the 90-m isobath. The upwelling jet is strongest over the upstream bank half, where it advects a tongue of dense water over the bank. There is a current reversal shoreward of the main jet at the bank center. Upwelling is most intense over the upstream part of the bank, while there is reduced upwelling and even downwelling over other bank sections. Downwelling-favorable winds create a near-bottom density front and a baroclinic jet (flowing in the direction of coastal-trapped wave propagation) that bend around the standard bank; the jet core moves from the 150-m isobath to the 100-m isobath and back over the bank. The downwelling jet is slowest and widest over the bank; there are no current reversals. Results over the bank are more similar to 2D results (that preclude alongshelf variability) than in the upwelling case. Downwelling is weakened over the bank. The density field evolution over the bank is fundamentally different from-the upwelling case. Most model results for banks with different dimensions are qualitatively similar to the standard run. The exceptions are banks having a radius of curvature smaller than the inertial radius; the main jet remains detached from the coast far downstream from these banks. The lowest-order across-stream momentum balance indicates that the depth-averaged flow is geostrophic. Advection, ageostrophic pressure gradients, wind stress, and bottom stress are all important in the depth-averaged alongstream momentum balance over the bank. There is considerable variability in alongstream momentum balances over different bank sections. Across-shelf and alongshelf advection both change the density field over the bank. Barotropic potential vorticity is not conserved, but the tendency for relative vorticity changes and depth changes to partially counter each other results in differences between the upwelling and downwelling jet paths over the bank. Only certain areas of the bank have significant vertical velocities. In these areas of active upwelling and downwelling, vertical velocities at the top of the bottom boundary layer are due to either the jet crossing isobaths or bottom Ekman pumping.
机译:这项研究研究了沿海银行如何影响分层大陆架上的风循环。对理想的对称库进行了数值实验。标准银行(长200公里,宽50公里)的尺寸类似于俄勒冈州大陆架上的Heceta Bank综合大楼。在10天的稳定风(0.1 Pa)下强制模型运行;比较上升流和下降流的情况。该库在电流和密度场中引入了明显的沿陆架变化。上升流有利的风产生上升流锋和斜压射流(与沿海岸陷波传播相反)(绕着标准堤岸弯曲),大约在等高线90米处。上升流射流在上游河岸半部最强,它在河岸上方平流着稠密的水。在银行中心,主射流有一个当前的反转向岸。在河岸上游,上升趋势最为剧烈,而在其他河岸部分,上升趋势甚至下降趋势也有所减少。向下气流有利的风形成了一个接近底部的密度锋和一个斜压射流(沿沿海陷波传播的方向流动)绕标准堤岸弯曲。射流核心从150米等深线移动到100米等深线,然后返回岸上。降流射流在河岸上最慢,最宽;目前没有逆转。与上升流情况相比,堤岸上的结果与二维结果(排除沿机架的可变性)更相似。银行的下跌趋势减弱。沿岸的密度场演化与上升流情况根本不同。不同规模银行的大多数模型结果在质量上都与标准运行相似。例外是曲率半径小于惯性半径的堤岸。主喷气机仍然远离这些堤坝下游的海岸。最低阶跨流动量平衡表明,深度平均流是地转的。对流,对流层压力梯度,风应力和谷底应力对于河岸沿流动量平衡的平均深度都很重要。不同河岸部分的沿河动量余额差异很大。跨层对流和沿层对流都改变了堤岸的密度场。正压势的涡度不是守恒的,但是相对涡度变化和深度变化部分抵消的趋势导致堤岸上流和下流射流路径之间的差异。银行只有某些区域具有明显的垂直速度。在活跃的上涌和下涌的这些区域中,底部边界层顶部的垂直速度是由于射流交叉等压线或底部埃克曼抽水所致。

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  • 来源
    《Journal of Physical Oceanography》 |2009年第6期|1273-1297|共25页
  • 作者单位

    Department of Marine Sciences, University of Connecticut, Groton, Connecticut Department of Marine Sciences, University of Connecticut, 1080 Shen-necossett Road, Groton, CT 06340-6097;

    College of Oceanic and Atmospheric Sciences, Oregon State University, Corvallis, Oregon;

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