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Wave-frequency flows within a near-bed vegetation canopy

机译:近床植被层内的波浪频流

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摘要

We study water flows and wave dissipation within near-bed pneumatophore canopies at the wave-exposed fringe of a mangrove forest on Cu Lao Dung Island, in the Mekong Delta. To evaluate canopy drag, the three-dimensional geometry of pneumatophore stems growing upward from the buried lateral roots of Sonneratia caseolaris mangroves was reconstructed from photogrammetric surveys. In cases where hydrodynamic measurements were obtained, up to 84 stems per square meter were observed, with stem heights < 0.6 m, and basal diameters 0.01-0.02 m. The parameter a = (frontal area of pneumatophores blocking the flow)/(canopy volume) ranged from zero to 1.8 m(-1). Within-canopy water velocity displayed a phase lead and slight attenuation relative to above-canopy flows. The phase lead was frequency-dependent, ranging from 0 to 30 degrees at the frequencies of energetic waves (> 0.1 Hz), and up to 90 degrees at lower frequencies. A model is developed for wave-induced flows within the vertically variable canopy. Scaling suggests that acceleration induced forces and vertical mixing were negligible at wave frequencies. Consistent with theory, drag-induced vertical variability in velocity scaled with A = T-w/(2 pi T-f), where T-w = wave period, T-f = 2/(C(D)a vertical bar u vertical bar) is the frictional time scale, CD; 1 2 is the drag coefficient, and vertical bar u vertical bar is a typical flow speed. For fixed wave conditions (vertical bar u vertical bar and T-w), theory predicts increasing dissipation with increasing vegetation density (i.e. increasing a), until a maximum is reached for order-one A. For larger A, within-canopy flow is so inhibited by drag that further increases in a reduce within-canopy dissipation. For observed cases, Lambda <= 0.38 at energetic wave frequencies, so wave dissipation near the forest edge is expected to increase with increasing pneumatophore canopy density. However, under different wave conditions, the most dense canopies may occasionally approach the dissipation maximum (Lambda approximate to 1). Predicted dissipation by the pneumatophore canopy was sufficient to attenuate most wave energy over distances slightly less (more) than 100 m into the marsh in 1 m (2 m) water depth.
机译:在湄公河德景的红树林的红树林的波浪暴露的森林的波浪暴露的边缘,我们将水流和波浪耗散研究。为了评估冠层阻力,从摄影测量调查重建了从Sonneratia Catelaris Mangroves的埋地侧根向上生长的气孔茎的三维几何形状。在获得流体动力学测量的情况下,观察到每平方米高达84个茎,茎高<0.6米,基底直径为0.01-0.02μm。参数A =(阻挡流量的颅骨面积)/(冠层体积)范围为0至1.8 m(-1)。内部内部水速显示相位引线和相对于上述篷布流动的轻微衰减。相位铅在频率依赖性,在能量波(> 0.1Hz)的频率下的0至30度,并且在较低频率下高达90度。为垂直可变顶篷内的波引起的波诱导流动开发了模型。缩放表明,在波频时,加速诱导力和垂直混合可以忽略不计。与理论一致,卷起速度的速度变化缩放为= tw /(2 pi tf),其中tw =波段,tf = 2 /(c(d)垂直条U垂直条)是摩擦时间尺度,CD;图1 2是拖动系数,垂直条U垂直杆是典型的流速。对于固定波条件(垂直条U垂直杆和TW),理论预测增加植被密度(即增加A),直到达到最大订单A.对于较大的A,在较大的A内,因此抑制了冠层通过阻力进一步增加,减少云机会耗散。对于观察到的情况,λ<= 0.38处为能量波频率,因此预计森林边缘附近的波浪耗散会随着气孔冠层冠层密度的增加而增加。然而,在不同的波条件下,最致密的檐篷可能偶尔接近耗散最大值(Lambda近似为1)。通过肺炎孔冠层预测的耗散足以在1米(2米)水深的沼泽中略微较低(更多)超过100μm的距离略低于100米。

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