An estimation of Ekman and geostrophic current over the Texas-Louisiana shelf

K. Yip, R. Reid
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引用次数: 1

Abstract

An estimation of wind driven Ekman current and geostrophic current over the Texas-Louisiana (TX-LA) continental shelf is demonstrated in this paper. One should expect the current field is a combination of two parts (G and E). Part G is the near surface part of the geostrophic current generated by the broad-scale wind over the shelf, plus possible influence from the offshore eddies. Part E is the near surface current produced by local Ekman dynamics. One should also expect that the direction and magnitude of part E is controlled by the local wind vector, while part G will tend to be constrained heavily by the local bathymetry of the shelf, which contributes the largest variance of the total near surface current. In order to indirectly obtain geostrophic current, the Ekman current can be determined using a direct calculation from the local wind stress vector. Since the local wind can be in any direction relative to the local shelf topography, a complex linear regression analysis statistical method to get the Ekman flow correctly over the shelf is used. The data set analyzed to obtain regression coefficient and correlation is simulated surface current time series at selected locations over the TX-LA shelf from September 10 to November 3, 2001, total 65 days in this "long" time series. The complex regression coefficient can also be expressed in polar form as a modulus and phase, where the phase gives the angle between the wind vector and the Ekman current vector. Negative angle representing clockwise rotation of the current vector from wind stress vector should be expected in the northern hemisphere. The observations from Texas Automated Buoy System (TABS) moorings R, B, F, D and J for this 55-day window are also used for comparison.
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德克萨斯州-路易斯安那大陆架上的埃克曼和地转流的估计
本文对德克萨斯-路易斯安那(TX-LA)大陆架上风驱动的埃克曼流和地转流进行了估算。我们应该预料到,流场是两部分(G和E)的组合。G部分是陆架上大尺度风产生的地转流的近地表部分,加上近海涡旋的可能影响。E部分为局部埃克曼动力学产生的近地表电流。人们还应该预料到,E部分的方向和大小是由当地的风矢量控制的,而G部分将倾向于严重地受到大陆架的当地水深的限制,这对总近地面电流的变化贡献最大。为了间接得到地转流,可以直接从局地风应力矢量计算出Ekman电流。由于当地风相对于当地陆架地形可以是任何方向,因此采用复线性回归分析统计方法来正确获得陆架上空的Ekman流。分析得到回归系数和相关性的数据集是2001年9月10日至11月3日在TX-LA大陆架上选定地点模拟的地表水流时间序列,在这个“长”时间序列中共65天。复回归系数也可以用极坐标形式表示为模量和相位,其中相位给出了风矢量和Ekman电流矢量之间的夹角。负角度表示当前矢量从风应力矢量顺时针旋转应该在北半球预期。德克萨斯州自动浮标系统(TABS)系泊处R、B、F、D和J的55天观测数据也用于比较。
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