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Submesoscale eddies near the Kuril Straits: Asymmetric generation of clockwise and counterclockwise eddies by barotropic tidal flow

机译:千岛海峡附近的亚中尺度涡:正压潮汐流不对称地产生顺时针和逆时针涡流

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摘要

High spatial resolution thermal infrared (TIR) images derived by the LANDSAT Thematic Mapper (TM) sensors show the presence of numerous small-scale eddies near the Kuril Islands. As the diameters of these eddies range from around 2 to 30 km (i.e., submesoscale), they are much smaller than the eddies previously reported in this region (several tens to some hundreds of kilometers in diameter). Our simulations suggest that small-scale eddies similar to those observed in the satellite data are generated by diurnal barotropic tides. The eddy generation is well defined from Etorofu/Friza to the Onnekotan Straits, and it is caused by the effects of coastal boundaries and the stretching of water columns, which lead to eddy growth even after eddies have left the coast. We find that the counterclockwise eddies are generally larger in number and size and stronger in vorticity and surface height than the clockwise eddies in both the gradient and cyclostrophic wind balance regimes. The possible causes of such asymmetry are (1) the effect of planetary-vorticity tube stretching, which can be significant even when the final relative vorticity becomes much greater than planetary vorticity and (2) asymmetric advection by the rotating tidal flow, which advects counterclockwise eddies offshore but clockwise eddies onshore. These eddies induce strong stirring with a maximum apparent diffusivity of 10^[8] cm2 s^[-1]. The numbers, properties, and mixing effects of eddies vary greatly with the spring-neap cycle.
机译:由LANDSAT主题映射器(TM)传感器获得的高空间分辨率热红外(TIR)图像显示出千岛群岛附近存在着许多小型涡流。由于这些涡流的直径范围约为2至30 km(即亚中尺度),因此它们比该地区先前报道的涡流要小得多(直径为几十到几百公里)。我们的模拟结果表明,与日卫星正压潮相比,与卫星数据中观测到的小涡旋相似。从埃托罗夫(Etorofu / Friza)到Onnekotan海峡,旋涡的产生是明确定义的,它是由沿海边界和水柱伸展引起的,即使旋涡离开了海岸,旋涡也导致旋涡的增长。我们发现,在梯度和回旋风平衡状态下,逆时针涡旋的数量和大小通常都比顺时针涡旋的数量和大小更大,涡旋和表面高度更强。这种不对称性的可能原因是(1)行星涡旋管拉伸的影响,即使最终相对涡旋远大于行星涡旋,该影响也很明显;(2)逆时针旋转的潮汐流引起的不对称对流。旋涡离岸,但顺时针旋涡在岸上。这些涡流引起强烈搅拌,最大表观扩散率为10 ^ [8] cm2 s ^ [-1]。涡流的数量,性质和混合效果随弹簧间隔的变化而变化很大。

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