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1.
基于长江河口1959-2011 年实测悬沙浓度数据,通过对河口最大浑浊带外围海域泥沙要素分析的基础上,研究了近期流域人类活动和河口整治工程对最大浑浊带悬沙浓度的影响。研究表明:① 流域人类活动对入海水量影响较小,无明显趋势变化,而沙量和含沙量呈现锐减趋势,也使得进入河口区域的泥沙量呈现一致锐减;② 长江口外海域和南部杭州湾海域悬沙浓度变化不大,北部苏北沿岸略有减小,因数值较长江口海滨区小约1 个数量级,对浑浊带影响较小;③ 最大浑浊带位置受径流和潮流控制,面积变化与入海沙量多寡关系密切;④ 整个浑浊带区域悬沙浓度受入海沙量锐减决定,2000-2009 年较1959-1999 年悬沙浓度减小约为24.73%,向海延伸减幅降低,且峰值区域向口内移动,泥沙再悬浮作用对维持最大浑浊带悬沙浓度起调节作用,但不能决定其锐减趋势;⑤ 北槽航槽最大浑浊带的悬沙浓度向海为低—高—低变化特点,受入海沙量锐减、北槽分流分沙比减少及床沙粗化等影响,使其上段和下段悬沙浓度减小趋势,而中段受南导堤越堤沙量的影响悬沙浓度呈增加趋势。 相似文献
2.
温州海区近岸表层水体悬沙分布及运动规律的遥感分析 总被引：4，自引：0，他引：4
利用Landsat-5/7卫星影像资料和实测含沙量资料,建立温州海区悬沙遥感模式,对表层水体悬沙分布及泥沙运动情况进行分析。研究表明,该海区水体表层平均含沙量较高,为0.1~0.3 kg/m3,受落潮流和N-NE向风浪作用及江浙沿岸流的影响,泥沙有自北向南沿岸输移的趋势,并在距浙江沿岸30~40 km范围内有一条明显的泥沙浑浊带,其范围由北向南逐渐减少,表层水体含沙量也由北向南逐渐降低,对浙江沿岸的泥沙运动产生重要影响。 相似文献
3.
许桂红 《中国地理与资源文摘》2003,(4)
建立了珠江口海域三维悬浮泥沙的非饱和输沙数学模型,并与珠江口三维水动力斜压模型耦合,对悬沙迁移分布进行了模拟。模型由4个点的逐时实测含沙量过程进行了 相似文献
4.
中国黄土分布区多沙曲流发育规律 总被引：1，自引：0，他引：1
依据中国黄土分布区多沙曲流的水沙资料、河床平面形态和河床大断面测量资料分析认为：多沙河流来水变率影响河床断面形态和曲流发育;由于窄深的河槽是高含沙水流输沙的必要条件和结果,因此随着含沙量的增加,多沙河流河床断面形态首先出现变窄深的趋势,随着含沙量的进一步增加,水流造床能力增大,河槽会向宽浅方向调整;一定的河床冲淤强度有利于曲流的发育,随着含沙量的增加,多沙河流河床曲率存在先增加后减小的规律。 相似文献
5.
依据中国黄土分布区多沙曲流的水沙资料、河床平面形态和河床大断面测量资料分析认为:多沙河流来水变率影响河床断面形态和曲流发育;由于窄深的河槽是高含沙水流输沙的必要条件和结果,因此随着含沙量的增加,多沙河流河床断面形态首先出现变窄深的趋势,随着含沙量的进一步增加,水流造床能力增大,河槽会向宽浅方向调整;一定的河床冲淤强度有利于曲流的发育,随着含沙量的增加,多沙河流河床曲率存在先增加后减小的规律. 相似文献
6.
长江口外海滨悬沙分布及扩散特征 总被引：8，自引：1，他引：8
长江口外海滨地区是陆海相互作用显著的区域,该区域复杂的水流等动力因素和地形条件决定了悬沙分布和扩散的特点。本文利用大量实测资料,对口外海滨地区悬沙的分布特征进行了综合分析,研究结果表明,平面分布不均,西高东低,南高北低,高低相差悬殊是长江口外水域悬沙平面分布的主要特点。枯季自西向东含沙量均匀减小,等值线分布较为稀疏。垂向涨落潮含沙量也表现出不同的分布特征,在口外的中西部水域垂向扩散系数较大,水体垂向混合程度均匀;垂向混合程度加强,水体含沙量也随之显著增加,这也造就了口外的南北两个高含沙区。 相似文献
7.
长江河口最大浑浊带的泥沙特性和输移规律* 总被引：19，自引：0，他引：19
本文通过对不同河段的泥沙特性和输移规律的对比分析,确认长江河口来沙丰富,在河口潮流不对称和重力环流的作用下,大量泥沙向滞流点辐聚,形成最大浑浊带。最大浑浊带含沙量高,泥沙絮凝沉速快。潮流强劲,引起床沙再悬浮,输沙能力强。长江河口最大浑浊带活动区与河口拦门沙位置基本一致。本研究成果对于加深认识河口拦门沙的成因和变化,以及航槽治理具有重大的现实间义。 相似文献
8.
9.
长江河口悬浮泥沙的混合过程 总被引：2，自引：0，他引：2
根据准同步观测的悬浮泥沙及表层沉积物粒度、流速、含沙量资料, 分析了长江口及临近海域悬浮泥沙在河口的混合过程。长江河口-陆架系统悬浮泥沙中值粒径呈现“细-粗-细”的变化规律, 河口上段悬浮泥沙中值粒径为8.9 μm, 拦门沙海域为10.5 μm, 陆架区为4.5 μm, 北支为9.9 μm, 杭州湾口为5.6 μm, 泥沙类型为粘土质粉砂。河口上段和陆架区悬浮泥沙与表层沉积物的垂向混合作用较弱, 拦门沙区域二者发生强烈的混合和交换, 悬浮泥沙在由长江河口向陆架系统输移过程中仅有表层泥沙保留了流域输入的泥沙粒度特征。长江口悬浮泥沙中值粒径与含沙量呈良好的正相关关系, 水流的剪切作用是引起拦门沙海域泥沙再悬浮、近底高含沙量和悬浮泥沙粒径增加的主要原因, 悬浮泥沙粒径和含沙量的增加主要由粉砂组分的增加引起。2007 年长江河口区范围内悬浮泥沙中值粒径比2003 年普遍减小11％, 含沙量比2003 年减小22%, 河口上段含沙量对流域来沙减少的响应最为敏感, 而拦门沙区的泥沙粒径对流域来沙减少的响应最敏感。在长江流域来沙量减少的背景下, 河口拦门沙区域仍能维持较高的含沙量, 主要缘于河口系统内部的供沙 相似文献
10.
特枯水情对长江中下游悬浮泥沙的影响 总被引：3，自引：0，他引：3
基于长江中下游气象资料、历史水沙资料和2006 年10 月现场水沙观测资料, 分析了 典型枯水年大通站的月均径流量和输沙率特征、2006 年特枯水情产生的气候背景以及对长江中下游含沙量和悬沙粒径产生的影响。分析表明, 枯水年长江干流输沙量有显著的减少, 2006 年特枯水情下大通站汛期输沙量仅占多年平均值(1985-2000 年) 的19.8%。在特枯水情 和三峡工程蓄水的背景下, 2006 年10 月长江中下游含沙量平均为0.057 kg/m3, 只占 2003-2005 年10 月平均值的20.6%。2006 年10 月长江中下游悬沙中值粒径平均为4.8 µm, 悬沙中值粒径只占多年平均值的26.3%, 占近期平均值的41.8%。含沙量、悬沙粒度和中游 河床冲淤特性的综合分析表明, 城陵矶-湖口河段水沙垂向交换强, 是三峡兴建以后近期河 道调整频繁的河段。洞庭湖和鄱阳湖对长江干流含沙量的贡献较大, 尤以鄱阳湖的贡献最大, 长江中下游其他支流对长江干流含沙量的贡献较小。汉江和巢湖对长江中下游悬沙粒径的影响相对较大, 而洞庭湖和鄱阳湖则对悬沙粒径的影响相对较小。 相似文献
11.
长江河口最大浑浊带水沙输运机制分析 总被引：33，自引：0，他引：33
本文根据大量的实测资料，运用机理的分析方法，讨论了长江口最大浑浊带中各输沙项的作用。结果表明，平均流输沙、斯托克斯漂流效应、潮汐捕集以及垂向不流是净输沙的主要部分。 相似文献
12.
我国沿海近岸带水域的悬沙分布特征 总被引：4，自引：1，他引：3
本文根据实测悬沙资料,阐述了我国沿海近岸带水域的悬沙浓度由黄河口和长江口-杭州湾为中心,分别向南、北递减,高低相间,构成波状起伏的分布特征,同时分析了径流输沙、潮流、波浪、海岸类型诸要素在悬沙浓度时空变化中的不同作用. 相似文献
13.
ADCP在长江口悬沙输运观测中的应用 总被引：12，自引：1，他引：11
声学多普勒流速剖面仪 (ADCP)是近年来发展起来的一种用于测量流速的声学仪器 ,同时还可以通过建立回声强度和现场取得水样的回归关系式而获得悬沙浓度的数据。本文利用在长江口两个站位的高频观测数据 ,对现场取得的悬沙作粒度分析 ,在此基础上对枯季长江口地区悬沙输送机制和悬沙粒度对水动力的响应进行了分析和探讨。结果表明 :平均流输运在整个悬沙输送中占主导地位 ,同时潮扩散和垂向扩散作用也是引起两站悬沙输运的重要因子 ;不同层次和不同时刻的悬沙粒度参数的变化 ,既和海 陆转换有关 ,也和潮相变化密切相关。 相似文献
14.
Suspended sediment load in the turbidity maximum zone at the Yangtze River Estuary:The trends and causes简 总被引：6，自引：2，他引：4
Based on the analysis of suspended sediment elements at estuaries, influence of human activities and estuarine regulation projects on the turbidity maximum zone was studied according to the measurement data between 1959 and 2011. It was found that human activi- ties had little effect on the seaward water while the sharp decrease of sediment volume and concentration in runoff led to the sharp decrease of turbidity maximum zone in the estuary. The concentration at outside sea and Hangzhou Bay did not change, and that along the Subei coast also decreased a little, which had no influence on the turbidity maximum zone. Com- pared with the concentration between 1959 and 1999, the peak of concentration moved up- stream in the estuary, and the concentration in 2000-2009 decreased by about 24.73% with a narrower variation range along the river to the sea. The suspended sediment concentration in North Passage was low in upstream and downstream because of the decrease of seaward sediment and coarsening of bed material, while it was relatively high in the middle due to the influence of sediment cross the north jetty. 相似文献
15.
Based on the analysis of suspended sediment elements at estuaries, influence of human activities and estuarine regulation projects on the turbidity maximum zone was studied according to the measurement data between 1959 and 2011. It was found that human activities had little effect on the seaward water while the sharp decrease of sediment volume and concentration in runoff led to the sharp decrease of turbidity maximum zone in the estuary. The concentration at outside sea and Hangzhou Bay did not change, and that along the Subei coast also decreased a little, which had no influence on the turbidity maximum zone. Compared with the concentration between 1959 and 1999, the peak of concentration moved upstream in the estuary, and the concentration in 2000-2009 decreased by about 24.73% with a narrower variation range along the river to the sea. The suspended sediment concentration in North Passage was low in upstream and downstream because of the decrease of seaward sediment and coarsening of bed material, while it was relatively high in the middle due to the influence of sediment cross the north jetty. 相似文献
16.
Karen Edelvang M.Sc. Michael Larsen M.Sc. assoc. prof. Morten Pejrup Ph.D. 《Geografisk tidskrift / udgivet af Bestyrelsen for Det Kongelige danske geografiske selskab》2013,113(1):116-119
Edelvang, Karen; Larsen, Michael; Pejrup, Morten: Tidal Variation in Field Settling Velocities of Suspended Sediment in a Tidal Channel. Geografisk Tidsskrift 92:116–121. Copenhagen 1992. Particles of silt and clay may form large, low density floes when suspended in salt water. The sediment floes have settling velocities much higher than the single small particles constituting them and therefore, the flocculation process may strongly influence the transport of cohesive sediment in estuarine environments. will be described in this paper, the field settling velocities of suspended sediment were investigated in a large tidal channel with tidal current velocities up to 1.3 m/s and depths of about 10 m. The analyses of suspended sediment were made on both bottom and surface samples. For the bottom samples, equivalent median fall diameters in the range 26–98 μm were measured. For surface samples, the range was 15–40 μm. During most of the tidal period, the occurrence of much larger settling diameters near the bottom was due to the suspension of individual sand and silt particles. For the investigated periods, high-tide was the only possible time to observe flocculation influencing the vertical distribution of finegrained sediment in the water column. 相似文献
17.
On the vertical structure of tidal currents in a homogeneous sea 总被引：15，自引：0，他引：15
Summary. The vertical variation of tidal currents caused by friction at the sea-bed is investigated in both qualitative and quantitative ways with the Coriolis force being taken into account. The simple model with the assumption of constant eddy viscosity is employed to study the effects of friction on the vertical structure of tidal currents. The model explains these effects in vertical change of the maximum velocity, the ellipticity (the ratio of the minor to the major axis) of current ellipse, the time and the direction of the maximum velocity, and the ratio of diurnal current to semidiurnal current.
To reach a quantitative agreement with the data observed by Bowden & Fairbairn in the Irish Sea, the mixing length theory is applied to numerical calculation of the vertical distribution of tidal currents with a finite difference scheme. A fair agreement with the observations is obtained in the calculation. The results show the following features: (1) the vertical profile of amplitude of the main component for the current is almost logarithmic throughout the depth; (2) the corresponding profde for the shearing stress is almost linear with depth; (3) the maximum stress lags the maximum velocity with the delay increasing with elevation; (4) the eddy viscosity coefficient has its maximum around the mid-depth; and (5) the vertically averaged viscosity lags the velocity magnitude.
The dependence of the quadratic resistance coefficient and the coefficient k defined by Bowden's formula = k hū(h — depth, and ū — depth-averaged eddy viscosity and velocity) on the roughness length is given for a steady flow in a non-rotating system. The numerical solution shows that these relations can be approximately applied to the tidal currents in shallow waters. 相似文献
To reach a quantitative agreement with the data observed by Bowden & Fairbairn in the Irish Sea, the mixing length theory is applied to numerical calculation of the vertical distribution of tidal currents with a finite difference scheme. A fair agreement with the observations is obtained in the calculation. The results show the following features: (1) the vertical profile of amplitude of the main component for the current is almost logarithmic throughout the depth; (2) the corresponding profde for the shearing stress is almost linear with depth; (3) the maximum stress lags the maximum velocity with the delay increasing with elevation; (4) the eddy viscosity coefficient has its maximum around the mid-depth; and (5) the vertically averaged viscosity lags the velocity magnitude.
The dependence of the quadratic resistance coefficient and the coefficient k defined by Bowden's formula = k hū(h — depth, and ū — depth-averaged eddy viscosity and velocity) on the roughness length is given for a steady flow in a non-rotating system. The numerical solution shows that these relations can be approximately applied to the tidal currents in shallow waters. 相似文献
18.
1998年 1 2月 1 1日至 1 999年 1月 1 3日在中山站近岸海域进行了一次较为全面的生态环境监测 ,监测内容包括∶ p H、T、盐度 (电导率 )、浊度、DO、COD、营养盐 (NO3 - N、NO2 - N、NH4 -N和 PO4 - P)和叶绿素 ,部分监测站位海水样品分层采集 ;其间还进行两次中山站区排污口生活污水连续 2 4小时监测。结果表明 ,冰缝间以及海冰底层下 1 m内的海水为各种环境理化因子的急剧变化层 ,大于冰底 1 m深的海水中的各要素变化梯度趋于平稳 ,营养盐垂直分布具有一定规律。p H和 DO为一类海水水质 ,无机氮属一、二类水质 ,无机磷属超三类水质 ,表层海水中叶绿素 a的平均值为 0 .6 71 mg/m3。中山站排放的生活污水中 COD、p H和悬浮物均符合我国的废污水排放标准 ,仅无机磷超一级排放标准。文中还探讨了在中山站近岸海域开展生态环境监测的监测方法 相似文献