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The influence of bed forms on reference concentration and suspension under waves and currents

机译:床形式对波动和电流下参考浓度和悬浮液的影响

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Hydrodynamic, suspension and bed-form measurements were made 2km off the Dutch coast near Noordwijk aan Zee in similar to 14 m water depth for a period of 32 days in 2003. Tidal currents were just able to suspend sand at the bed at peak spring tide but most suspension and transport occurred as a result of the combination of waves and currents. Burst-average (17 min) sand concentration profiles (C-profiles) from an acoustic backscatter instrument were used to define the (varying) location of the sea-bed, following the method used by Green et al. [Green, M.O., Dolphin, T.J., Swales, A., Vincent, C.E., 1999. Transport of mixed-size sediments in a tidal channel. Coastal Sediments '99, edited by N.C. Kraus, and W.G. McDougal, ASCE, Long Island, New York, pp. 644-6581. Reference concentrations at the sea-bed (CO) and at 1 cm (C-1) were examined in relation to both the hydrodynamic conditions and the type of bed forms present. The C-0 predictive equations of Green and Black [Green, M.O., Black, K.P., Suspended sediment reference concentration under waves: field measurements and critical analysis of two predictive models, Coastal Engineering, 38, 115-141,1999](short-wave ripples) and Nielsen [Nielsen, P., Suspended sediment concentrations under waves, Coastal Engineering, 10, 23-31, 19861(all bed forms; includes ripple steepness), both of which require knowledge of the bed-form type, were not as successful in explaining the variance in our Co data as a regression of Co against the skin-friction Shields parameter theta'(cw) that ignored bed-form type (73% of variance explained). The values of the reference concentration C, were compared with the Lee et al. [Lee, G.-H., Dade, W.B., Friedrichs, C.T., Vincent, C.E., Examination of Reference Concentration Under Waves and Currents on the Inner Shelf, Journal of Geophysical Research, 109, 1-10, 2004] equation which predicts C, from the product of the Shields parameter and the inverse Rouse parameter; 51% of the variance in C, was explained. The shapes of the C-profiles were very variable as reported by Dolphin et al. [Dolphin, T.J., Grasmeijer, B.T.Vincent, C.E., Sand suspension due to waves and tidal flow over short and long-wave ripples and flat beds on the Dutch Coast, in Sand Transport and Morphology of Offshore Mining Pits, edited by L.C. van Rijn, R.L. Soulsby, P. Hoekstra, and A.G. Davies, Aqua Publications, Amersfoort, The Netherlands, 2005.]., particularly over larger and steeper bed forms when the position of the measurements in relation to the bed-form geometry became important. However, a Rouse-shaped profile (in which the sediment diffusivity increases linearly with height) could be fitted (R-2 > 95%) to the lowest 0.2 m of 89% of the suspended sand profiles. The apparent separation of C-profiles, when grouped by bed-form type, is due to the variation in the reference concentration and not to the dependence on the friction velocity, which shows large scatter and no systematic variation with bed-form type. It is concluded that, for most practical applications, reference concentration at I cm can be predicted by Lee et al. [Lee, G.-H., Dade, W.B., Friedrichs, C.T., Vincent, C.E., 2004. Examination of Reference Concentration Under Waves and Currents on the Inner Shelf., Journal of Geophysical Research, 109, 1 -10.] and that the suspended sediment profiles are Rouse-shaped with a shape parameter p of 0.80 +/- 0.25; knowledge of the bed-form type does not, at the Noordwijk site, help to refine either the reference concentration or the shape of the suspended concentration profiles. (C) 2009 Elsevier Ltd. All rights reserved.
机译:在2003年,在Noordwijk aan Zee附近的荷兰海岸附近2公里处以大约14 m的水深进行了水动力,悬浮和床形测量,为期32天。潮汐流只能在春季潮汐峰值时将沙子悬浮在河床上。但是大多数的悬浮和运输都是由于波浪和水流的结合而发生的。按照格林等人的方法,使用声学反向散射仪的爆炸平均(17分钟)砂浓度剖面(C剖面)来定义海床的(变化)位置。 [Green,M.O.,Dolphin,T.J.,Swales,A.,Vincent,C.E.,1999.潮汐通道中混合大小沉积物的运输。 《海岸沉积物99》,由N.C. Kraus和W.G. McDougal编辑,ASCE,纽约长岛,第644-6581页。检查了海床(CO)和1 cm(C-1)处的参考浓度,同时考虑了流体动力学条件和存在的床型类型。 C-0 Green和Black的C-0预测方程[Green,MO,Black,KP,波浪下的悬浮泥沙参考浓度:现场测量和两种预测模型的临界分析,Coastal Engineering,38,115-141,1999](short-波浪波纹)和尼尔森[Nielsen,P.,波浪下的悬浮泥沙浓度,海岸工程,10,23-31,19861(所有床形;包括波纹陡度),这两个都需要了解床形类型。在解释Co数据中的方差方面,没有像Co对忽略床型的皮肤摩擦Shields参数theta'(cw)的回归那样成功地解释了Co(方差的73%)。将参考浓度C的值与Lee等人进行了比较。 [Lee G.-H.,Dade,WB,Friedrichs,CT,Vincent,CE,内层波和流下参考浓度的检验,地球物理研究杂志,109,1-10,2004] C,由Shields参数和Rouse逆参数的乘积得到;解释了C中51%的方差。如Dolphin等报道的,C型轮廓的形状变化很大。 [L.C.编辑,《近海采矿坑的沙子运输和形态学》,由荷兰海岸的短波和长波波纹以及平坦的床层上的波浪和潮汐流引起的沙子悬浮,T.J.,Grasmeijer,B.T。Vincent,C.E.。 van Rijn,RL Soulsby,P。Hoekstra和AG Davies,Aqua Publications,荷兰阿默斯福特,2005年。],特别是在相对于床形几何尺寸的测量位置变得重要时,在更大,更陡的床形上。但是,可以将Rouse形剖面(沉积物扩散率随高度线性增加)(R-2> 95%)安装到89%悬浮砂剖面中最低的0.2 m。当按床形类型分组时,C形轮廓的明显分离是由于参考浓度的变化,而不是由于对摩擦速度的依赖性,这显示了较大的散布,并且没有随床形类型的系统性变化。结论是,对于大多数实际应用,Lee等人可以预测1 cm处的参考浓度。 [Lee G.-H.,Dade,WB,Friedrichs,CT,Vincent,CE,2004年。内层波浪和电流作用下的参考浓度检验,地球物理研究杂志,109,1 -10。]悬浮的沉积物剖面呈Rouse形,形状参数p为0.80 +/- 0.25;在诺德韦克(Noordwijk)站点,对床型的了解并不能帮助完善参考浓度或悬浮浓度曲线的形状。 (C)2009 Elsevier Ltd.保留所有权利。

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