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首页> 外文期刊>Continental Shelf Research: A Companion Journal to Deep-Sea Research and Progress in Oceanography >Acoustic turbulence measurements of near-bed suspended sediment dynamics in highly turbid waters of a macrotidal estuary
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Acoustic turbulence measurements of near-bed suspended sediment dynamics in highly turbid waters of a macrotidal estuary

机译:潮汐河口高混浊水中近床悬浮泥沙动力学的声湍流测量

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摘要

Sediment-turbulence interactions near the bed are still poorly understood in highly turbid estuaries, especially in the presence of fluid mud layers. This results primarily from the difficulty in measuring co-located velocity and suspended sediment concentration (SSC) at sufficiently high rate to resolve small turbulent flow scales. In this paper, we show how a set of commercial acoustic and optical backscattering systems known as ADCPs, ADVs and OBSs, can be deployed and used in a complementary way to perform large-scale profilings of tidal current and SSC combined with high-resolution velocity and SSC measurements in the highly turbid near-bed zone. The experiment was done in the Gironde estuary (France) which is well known for its turbidity maximum zone characterized by high SSC values, above 1 g l~(?1) near the surface. A first simple inversion method is proposed to convert the backscattered acoustic intensity measured with ADV into SSC data in the highly turbid near-bed zone. Near-bed SSC data from the OBS are used to compensate for the important acoustic sediment attenuation effect at an acoustic frequency of 6 MHz. No a priori knowledge of acoustic backscattering properties of mud suspensions is required with this calibration procedure. We obtain an attenuation coefficient for mud suspensions of 0.28 m~2/kg at 6 MHz leading to a good agreement between the SSC timeseries from the three ADV receivers and the OBS over the entire tidal cycle. The obtained SSC data are then analyzed with respect to the near-bed velocity, Reynolds shear stress and turbulent kinetic energy (TKE) timeseries in order to identify the relevant sediment transport processes during the tidal cycle. Significant differences in bed shear stress and TKE levels are found between ebb and flood stages with effects on near-bed sediment dynamics. During the ebb, maximum levels of tidal current, bed shear stress and TKE are associated with a reduction of near-bed sediment concentration (from 400 kg m~(?3) down to 100 kg m~(?3)). Bed liquefaction process is assumed to occur at this moment with the presence of highly concentrated mud layer and a possible lutocline at a distance of less than 20 cm above the bed. During the first 1.5 h of flood, turbulent activity remains moderate. The near-bed flood current is then inhibited very abruptly while a sudden increase in SSC occurred above the bed. Assuming that the ADV is able to estimate relevant turbulent erosion fluxes, the co-located velocity and SSC are multiplied and compared with settling flux measurements made onboard under quiescent water conditions. The mean sediment settling fluxes (averaged over 3 min) increase with SSC and are in relative good coherence with fluxes in quiescent water below the hindered regime, for SSC below 15 g l~(?1). Reducing averaging time from 3 min to 30 s allows to increase the range of turbulent fluxes and SSC values, up to 99 g l~(?1). At this scale, fluxes keep increasing quasi-linearly at higher SSC, suggesting the inhibition (delay or reduction) of the hindered settling regime as previously shown by Gratiot et al. (2005) from laboratory experiments. However, the 3-min averaged concentration field remained too low to conclude definitively on the effectiveness of such a process. Further analysis conducted at higher SSC regimes and under fully verified equilibrium are necessary.
机译:在高度浑浊的河口,尤其是在存在流体泥浆层的情况下,对床附近沉积物-湍流的相互作用仍然知之甚少。这主要是由于难以以足够高的速率测量并置速度和悬浮沉积物浓度(SSC)来解决小湍流水垢。在本文中,我们展示了如何部署和使用一套商业上的声学和光学反向散射系统,称为ADCP,ADV和OBS,以互补的方式进行潮汐流和SSC的大规模剖析以及高分辨率速度高度混浊的近床区进行SSC和SSC测量。该实验是在吉伦特河口(法国)进行的,该河口以浊度最大区为特征,其最大SSC值高​​,在地面附近1 g l〜(?1)以上。提出了第一种简单的反演方法,将在高浊度近床层中利用ADV测量的反向散射声强转换为SSC数据。来自OBS的近床SSC数据用于补偿6 MHz声频下重要的声沉积物衰减效应。通过该校准程序,不需要泥浆悬浮液的声学反向散射特性的先验知识。我们获得了在6 MHz下泥浆悬浮液的衰减系数为0.28 m〜2 / kg,从而导致在整个潮汐周期中来自三个ADV接收器的SSC时间序列与OBS之间的一致性良好。然后针对近床速度,雷诺剪切应力和湍动能(TKE)时间序列对获得的SSC数据进行分析,以识别潮汐周期中的相关泥沙输送过程。在潮退期和洪水期之间,床剪切应力和TKE水平存在显着差异,对近床沉积物动力学有影响。在退潮期间,最大的潮流,河床剪应力和TKE与近床沉积物浓度的降低有关(从400 kg m〜(?3)降至100 kg m〜(?3))。假定此时液化过程发生在高度浓缩的泥浆层和可能存在的卢比克林在距床不到20厘米的距离处。在洪水的前1.5小时内,湍流活动保持中等水平。然后,在床层上方SSC突然增加的同时,突然抑制了近床层洪水电流。假设ADV能够估算出相关的湍流侵蚀通量,则将同位速度和SSC相乘,并与在静态水条件下在船上进行的沉降通量测量结果进行比较。对于低于15 g l〜(?1)的SSC,平均沉积物沉降通量(平均超过3分钟)随SSC的增加而增加,并且与静态水在受阻状态下的通量具有较好的一致性。将平均时间从3分钟减少到30 s,可以将湍流和SSC值的范围增加到99 g l〜(?1)。在这个规模上,通量在较高的SSC时保持准线性增加,这表明了受阻沉降机制的抑制(延迟或减少),如Gratiot等人先前所述。 (2005)来自实验室实验。但是,3分钟的平均浓度场仍然太低,无法确切地确定这种方法的有效性。有必要在较高的SSC体制下以及经过充分验证的平衡下进行进一步分析。

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