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首页> 外文期刊>Journal of Physical Oceanography >Estuarine Boundary Layer Mixing Processes: Insights from Dye Experiments
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Estuarine Boundary Layer Mixing Processes: Insights from Dye Experiments

机译:河口边界层混合过程:染料实验的见解

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A series of dye releases in the Hudson River estuary elucidated diapycnal mixing rates and temporal variability over tidal and fortnightly time scales. Dye was injected in the bottom boundary layer for each of four releases during different phases of the tide and of the spring-neap cycle. Diapycnal mixing occurs primarily through entrainment that is driven by shear production in the bottom boundary layer. On flood the dye extended vertically through the bottom mixed layer, and its concentration decreased abruptly near the base of the pycnocline, usually at a height corresponding to a velocity maximum. Boundary layer growth is consistent with a one-dimensional, stress-driven entrainment model. A model was developed for the vertical structure of the vertical eddy viscosity in the flood tide boundary layer that is proportional to u_*~2/N_∞, where u_* and N_∞ are the bottom friction velocity and buoyancy frequency above the boundary layer. The model also predicts that the buoyancy flux averaged over the bottom boundary layer is equal to 0.06N_∞u_*~2 or, based on the structure of the boundary layer equal to 0.1N_(BL)u_*~2, where N_(BL) is the buoyancy frequency across the flood-tide boundary layer. Estimates of shear production and buoyancy flux indicate that the flux Richardson number in the flood-tide boundary layer is 0.1-0.18, consistent with the model indicating that the flux Richardson number is between 0.1 and 0.14. During ebb, the boundary layer was more stratified, and its vertical extent was not as sharply delineated as in the flood. During neap tide the rate of mixing during ebb was significantly weaker than on flood, owing to reduced bottom stress and stabilization by stratification. As tidal amplitude increased ebb mixing increased and more closely resembled the boundary layer entrainment process observed during the flood. Tidal straining modestly increased the entrainment rate during the flood, and it restratified the boundary layer and inhibited mixing during the ebb.
机译:哈德逊河河口的一系列染料释放阐明了潮汐和两周时间尺度上的二叠氮混合速度和时间变化。在潮汐和春季小憩周期的不同阶段,针对四个释放中的每一个,在底部边界层中注入了染料。斜向混合主要通过夹带发生,夹带由底部边界层中的剪切产生驱动。泛滥时,染料垂直延伸穿过底部混合层,并且在比浓可可碱附近,其浓度突然降低,通常在与速度最大值相对应的高度。边界层的增长与一维应力驱动的夹带模型一致。建立了潮汐边界层垂直涡粘性垂直结构的模型,该模型与u_ *〜2 /N_∞成比例,其中u_ *和N_∞是边界层上方的底部摩擦速度和浮力频率。该模型还预测,在底部边界层上平均的浮力通量等于0.06N_∞u_*〜2,或者基于边界层的结构等于0.1N_(BL)u_ *〜2,其中N_(BL )是整个潮汐边界层的浮力频率。剪切力和浮力通量的估计值表明,潮汐边界层的通量理查森数为0.1-0.18,与模型一致,表明通量理查森数为0.1-0.14。在退潮期间,边界层更加分层,其垂直范围没有洪水泛滥时那样清晰。在潮汐退潮期间,由于底部压力减小和分层稳定,退潮期间的混合速率明显弱于洪水。随着潮汐振幅的增加,潮汐混合增加,并且更类似于洪水期间观察到的边界层夹带过程。潮汐应变适度增加了洪水期间的夹带率,并重新界定了边界层并在退潮期间抑制了混合。

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