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Boundary layer velocity structure in a coldwater coral area of Haddock Channel, southwest Grand Banks.

机译:西南大河岸Haddock海峡冷水珊瑚区的边界层速度结构。

摘要

Gorgonian corals occur extensively at continental slope depths > 200 m off the southwestudGrand Banks of Newfoundland. Among these corals, Keratoisis grayi formsudgorgonian coral thickets on cobbles and boulders in otherwise muddy sand habitats.udThese thickets are believed to form a critical benthic habitat, in particular for juvenileudfish, and as such are an integral part of the ecosystem. These coral thickets areudimpacted by bottom trawling activity which therefore could have far reaching consequencesudfor the larger ecosystem. This thesis reports on a study of how the oceanudbottom boundary layer is affected by the presence of coral thickets. This informationudis important both to establish the characteristics of coral habitat but also to demonstrateudhow the removal of corals modifies the boundary layer which would in turnudmodify the benthic environment.udBottom boundary layer currents in coral habitat in Haddock Channel were characterizedudusing two 2-MHz acoustic Doppler current profilers.The profilers were deployedudon the seafloor at a depth of 700 m, looking upward, for 85 hours, beginningudJuly 17th, 2007. The effective vertical profiling range was 4 meters, with 1 meteruddepth resolution, sampling every 2.7 minutes. One instrument was placed in an areaudwhere bamboo corals (Keratoisis grayi ) extend approximately to 1 meter in heightudand occur with a density on the order of 1 colony per square meter (Coral Site). Theudsecond instrument was deployed 100 meters away in an area with visually similar sea floor characteristics, but from which the corals had been removed by a researchudbottom trawl (Mud Site). Mean flow speeds at both the Mud and Coral Site areudon the order of 10 cm s⁻¹, which is consistent with previous current data from theudgeneral area. Observed currents showed some evidence of tidal forcing but other nonlinearudprocesses clearly influence the current regime. Speed profiles were fitted to theudlogarithmic law of the wall to obtain bottom roughness zₒ, and friction velocity u∗udestimates. Both the Mud and Coral Site appear to conform to the logarithmic law ofudthe wall for turbulent boundary layers.udFriction velocity (u∗) estimates at flow speeds less than 5 cm s⁻¹, were consistentlyudhigher at the Coral Site, relative to the Mud Site; Mud Site u∗ values were 30%udto 80% of Coral Site estimates, indicating increased turbulence due to the presenceudof corals. However, friction velocity increased faster with flow speed at the MududSite, suggesting that at higher flow speeds coral induced bottom roughness is lessudimportant to friction velocity. There was significant uncertainty in bed roughnessudestimates, however bed roughness values at the Coral Site (mean zₒ = 0.51 ± 0.28udcm), were found to be generally higher at flow speeds below 5 cm s⁻¹, compared toudthe Mud Site (mean zₒ = 0.27 ± 0.40 cm), again possibly indicating that the coraludare affecting the hydrodynamic roughness at low speeds.udBackscatter intensity was also examined as an indication of suspended organicudmaterial. It was impossible to make relative absolute comparisons between the twoudsites but relative changes in backscatter intensity could be compared. Backscatterudlevels from both sites increased as flow speeds increased, up to 7 cm s⁻¹. Backscatterudincreased faster with flow speed at the Mud Site, relative to the Coral Site, for speedsudbetween 2.5 and 7 cm s⁻¹, which is broadly consistent with the suggestion of greaterudincrease in friction velocity values seen at the Mud Site.udAbove 7 cm s⁻¹, Coral Site backscatter intensity increased substantially, while the corresponding Mud Site backscatter intensity declined. The reason for this change inudtrend is unclear, a possible explanation being a transition into a different flow regimeudwhereby increased flow speeds interact favourably with the rough topography createdudby the corals. However, the large uncertainty estimates for backscatter levels at theseudhigher speeds were such that it was very difficult to draw firm conclusions.udWe conclude that higher u∗ and zₒ estimates at low flow speeds at the Coral Site,udrelative to the Mud Site, are consistent with the hypothesis that the enhancement ofudturbulence due to the coral behaving as roughness elements is significant only at lowudflow speeds, enabling coral polyps greater opportunities to extract organic materialudfrom the water column due to resuspension of organic material from the sea floor.
机译:高更珊瑚广泛分布在距纽芬兰西南 ud大河岸200 m以上的大陆坡深度。在这些珊瑚中,喀拉托邦灰皮在原本是泥泞的沙地栖息地的鹅卵石和巨石上形成了 udgorgonian珊瑚丛。 。这些珊瑚丛受到底部拖网活动的影响,因此可能对更大的生态系统产生深远的影响。本论文报道了关于珊瑚礁的存在如何影响海底边界层的研究。这些信息对于建立珊瑚栖息地的特征非常重要,也有助于证明去除珊瑚如何改变边界层进而反过来改变底栖环境。 ud对哈多克海峡珊瑚栖息地的底部边界流进行了表征。 使用两个2 MHz的声学多普勒电流剖面仪。剖面仪从2007年7月17日开始,在海底深度700 m向上部署85小时,有效垂直剖面范围为4米, 1米深的分辨率,每2.7分钟采样一次。将一种仪器放置在竹珊瑚(Keratoisis grayi)延伸至大约1米高的区域中,并且密度约为每平方米1个菌落(珊瑚地)。这个 udsecond仪器被部署在距离海底特征相似的区域100米处,但是珊瑚被研究用 udbottom拖网(Mud Site)移除。泥浆和珊瑚部位的平均流速都在10厘米s -1的数量级,这与以前来自“预算地区”的最新数据是一致的。观察到的电流显示了一些潮汐强迫的证据,但其他非线性明显过程明显影响了当前状况。将速度曲线拟合到墙的“ ”对数定律,以获得底部粗糙度z ^和摩擦速度u desuttimates。泥浆和珊瑚部位都似乎符合 udthe壁对湍流边界层的对数定律。 ud在流速小于5 cms⁻¹时的摩擦速度(u ∗)估计值在珊瑚部位始终一致高于相对于泥浆站点;泥位u *值是珊瑚位点估计值的30%至80%,表明由于存在珊瑚而导致湍流增加。但是,在Mud udSite处,摩擦速度随流速的增加而加快,这表明在较高流速下,珊瑚引起的底部粗糙度对摩擦速度的影响较小。床的粗糙度/脱附率存在显着的不确定性,但是发现,在低于5 cm s¹的流速下,珊瑚部位的床粗糙度值(平均zₒ= 0.51±0.28 udcm)通常更高。位置(平均zₒ= 0.27±0.40 cm),再次可能表明珊瑚在低速下会影响水动力粗糙度。 ud后向散射强度也被视为悬浮的有机材料的指示。不可能在这两个位置之间进行相对绝对比较,但是可以比较反向散射强度的相对变化。随着流速的增加,两个站点的反向散射 ud水平都增加,直至7 cm s¹。相对于珊瑚部位,泥浆部位的后向散射/流动速度更快,相对于珊瑚部位,速度在2.5至7 cm s¹¹之间,这与在泥浆部位看到的摩擦速度值较大或增加的建议基本一致在7 cm s¹以上,珊瑚站点的背向散射强度显着增加,而相应的泥浆站点的背向散射强度下降。这种趋势变化的原因尚不清楚,一个可能的解释是过渡到不同的流态中,从而增加的流速与珊瑚所形成的粗糙地形相互作用良好。但是,在这些较高的速度下,对背向散射水平的较大不确定性估计使得很难得出明确的结论。 ud我们得出的结论是,在低流速下,珊瑚站点的u ∗和zₒ估计较高,与泥浆相比该位点与以下假说相符,即珊瑚在低流速下仅表现为粗糙元素而引起的湍流增加,使得珊瑚息肉由于有机物的再悬浮而有更多机会从水柱中提取有机物。从海底。

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    Fowler William A.;

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