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1.
太湖水体中悬浮物的静沉降特征   总被引:8,自引:0,他引:8  
陈鋆  高光  李一平  王珂  逢勇 《湖泊科学》2006,18(5):528-534
本文分别采用斯托克斯沉降速率公式和重复深度吸管法计算了2005年4月、5月间在太湖进行的四次静沉降模拟实验中的沉降速度.结果表明:1)太湖水体中悬浮物的沉降属于絮凝沉降.2)水体中悬浮物浓度与沉降时间均呈现出明显的指数衰减规律(R~2>0.80),悬浮物中无机物含量较高时这种规律更为明显(R~2≥0.99).3)悬浮物浓较低时,太湖悬浮物的沉降速率与水体中的悬浮物浓度无明显的相关关系;而悬浮物浓度较高时,沉降速率随悬浮物浓度升高而增大.经拟合沉降速度(ω)与悬浮物浓度(C)之间符合Logistic曲线ω=0.021/(1 exp(-0.026(C-166.3))),R~2=0.98,n=54.4),斯托克斯公式可用来粗略估算太湖悬浮物的沉降速率,而重复深度吸管法则适合于较精确地计算太湖悬浮物的沉降速率.但在计算时须注意根据悬浮物的特性,选取其特征沉降速率.本文计算得到的太湖悬浮物的沉降速率范围为0.002 cm/s-0.005 cm/s.  相似文献   

2.
胡耀躲  张运林  杨波  张毅博 《湖泊科学》2018,30(4):992-1003
总悬浮物是水体中重要的光学敏感物质之一,很大程度上决定了水柱中光的吸收、散射和衰减,同时吸附营养盐、重金属和有毒有害物,对水体物质生物地球化学过程、沉积物埋藏动力和湖泊环境演化具有重要的意义.基于星地同步实验和静止水色成像仪GOCI(Geostationary Ocean Color Imager)构建了太湖悬浮物浓度估算模型,并分析了典型风浪过程中太湖悬浮物浓度短期动态变化过程.研究表明:对太湖水体悬浮物浓度较为敏感的波段为GOCI的第7波段(745nm)和第8波段(865 nm),悬浮物浓度与对应波段遥感反射率线性相关决定系数分别为0.72和0.55;基于GOCI第7波段的悬浮物浓度单波段遥感估算模型能较为准确地估算太湖的悬浮物浓度,模型相对均方根误差和平均绝对百分误差分别为28.3%和24.4%.通过研究典型风浪过程前后太湖悬浮物浓度变化发现其短期动态变化显著,风速、风向是悬浮物浓度短期动态变化的重要驱动因素,悬浮物浓度与风速呈正比,并随着风向扩散;高频连续GOCI影像结果显示悬浮物浓度短期动态变化对风浪扰动的响应有一定的滞后性,滞后时间为数小时到1天,悬浮物沉降与沉积物再悬浮的临界风速约为3.4 m/s.  相似文献   

3.
基于反射光谱和模拟MERIS数据的太湖悬浮物遥感定量模型   总被引:28,自引:5,他引:23  
吕恒  李新国  江南 《湖泊科学》2005,17(2):104-109
利用地物光谱仪研究了太湖水体的反射光谱特征,通过对比分析,发现580nm反射率值和810nm的反射峰高是太湖悬浮物的敏感波段,并通过光谱微分的方法,发现840nm附近的一阶微分与悬浮物浓度相关性最好,基于上述结论,分别建立了太湖悬浮物的反射光谱和一阶微分遥感定量模型,并利用反射光谱数据,模拟MERIS数据的波段设置,结果表明MERIS第5、12、13波段可以很好的估测太湖的悬浮物浓度.  相似文献   

4.
水动力条件下太湖透明度模拟研究   总被引:6,自引:0,他引:6  
根据太湖实测资料分析得到了太湖悬浮物浓度和透明度之间呈现明显的反比关系, 归纳总结了以往研究成果中建立的太湖透明度与悬浮物浓度之间的关系, 说明可以通过模拟太湖悬浮物来反映太湖透明度的变化规律. 实测资料表明, 不同水深处的悬浮物浓度与风速的变化趋势大致相近, 风速越大, 悬浮物浓度越大. 太湖波浪、湖流与悬浮物浓度均呈现正相关关系, 悬浮物浓度随着波浪和湖流的增大而增大, 但波浪是影响底泥再悬浮的主要因素, 流速次之. 建立了太湖湖流、波浪和悬浮物耦合的数学模型, 在悬浮物模型中考虑了波浪和湖流的综合影响. 并将床面层附近底泥的起悬量和沉降量分开处理, 考虑了近底水流中湍流脉动的随机特性, 引入了底泥起悬条件. 模型清楚地反映出了悬浮物中的底泥颗粒与床面层内运动底泥及床面活动底泥发生相互交换过程中的两个方面. 模拟结果表明太湖悬浮物沿岸区域受湖流的影响较大, 湖心区域受波浪影响较大. 利用该模型, 模拟了太湖悬浮物和透明度的变化规律, 模拟结果被实测值较好验证, 说明所建立的模型是基本合理的, 可用来进行太湖透明度的模拟和预测.  相似文献   

5.
秋季太湖悬浮物高光谱估算模型   总被引:10,自引:0,他引:10  
2004年10月,在太湖设置67个采样点,现场测量了水体遥感反射比、后向散射系数和辅助参数,实验室分析了水体的悬浮物浓度和水色要素吸收系数.本文在对遥感反射比光谱分析的基础上,比较了几种水体遥感反射比光谱估算悬浮物浓度的方法,结果发现广泛应用的带比值项的算法,虽然可以应用于太湖总悬浮物浓度估算,但是普遍存在相对误差较高的弱点.通过对光谱的分析,确定了750hm单波段算法的参数,并提出了利用近红外812nm波峰高度来估算水体悬浮物的方法.文中还详细阐述了为什么比值算法等在太湖水体悬浮物浓度估算中相对误差比较高,并解释了利用近红外估算精度高的原因,并指明以上算法在遥感应用中的优点和不足,以及现实水体(水质)遥感对现有遥感器配置和遥感算法的需求.  相似文献   

6.
基于叶绿素荧光峰特征的浑浊水体悬浮物浓度遥感反演   总被引:4,自引:0,他引:4  
周冠华  杨一鹏  陈军  李京 《湖泊科学》2009,21(2):272-279
内陆水体光学特性复杂,其水质参数遥感反演是当前环境遥感研究的热点与难点.2004年10月在太湖实测了67个站点的遥感反射率与相应站点水质参数浓度,通过对水体反射率光谱的分析发现,秋季太湖悬浮物主导了水体光学特性,叶绿素荧光峰的特征主要体现为悬浮物浓度的变化.据此建立了基于水面实测岛光谱遥感反射率数据的叶绿素荧光峰特征与悬浮物浓度之间的拟合关系,发现二者具有很好的响应关系.具体分析了叶绿素荧光峰绝对高度、基线高度、归一化高度(分别归一化到560nm附近最大反射率波段与近红外810nm附近最大反射率波段)及荧光峰积分面积(包括积分总面积、基线以下面积与基线以上面积)等儿种光谱特征与悬浮物浓度之间的关系,其相关系数(R2)分别为0.8822、0.7483、0.8901、0.8547、0.8927、0.8877、0.8632,平均相对误差分别为27.25%、41.03%、27.11%、25.75%、24.91%、25.47%、27.54%.总体反演精度较高,其中总积分面积法效果最好,基线高度法效果最差,而叶绿索荧光峰波段的位移与悬浮物浓度之间不存在明显的相关性.研究结果表明叶绿素荧光峰特征在浑浊内陆水体悬浮物浓度信息提取中具有很好的应用前景,该方法可为浑浊的二类水体悬浮物遥感反演提供了一个新思路.  相似文献   

7.
沉降运动是悬浮物主要运动形式之一,是影响营养盐内源释放的主要运动过程,研究悬浮物沉降速度对湖泊富营养化的研究具有重要意义.为了解浅水湖泊悬浮物的沉降特征,以太湖梅梁湾为例,采用声学多普勒流速仪,光学后向散射浊度仪以及风速风向仪在梅梁湾进行了连续9 d的野外观测.采用扩散沉降平衡的方法计算小风速情况下悬浮物的沉降速度,并对沉降速度与垂向流速、风速、悬浮物浓度的关系进行分析.结果表明悬浮物平均沉降速度为0.0785 mm/s,表层垂向流速和悬浮物浓度对悬浮物沉降速度变化起主要作用;而在底层,风速、垂向流速、悬浮物浓度都对悬浮物运动有重要影响,具体表现为风速1.5 m/s时,垂向流速紊动增大,悬浮物因起悬而浓度较大,并且沉降速度波动较大;风速1.5 m/s时,垂向流速基本向下且流速较小,沉降速度也较小.本文揭示了大型浅水湖泊悬浮物的动态沉降特征,为今后太湖污染物的输移、水环境数学模型和湖泊富营养化的深入研究奠定了必要的基础.  相似文献   

8.
太湖沉积物再悬浮模拟方法   总被引:16,自引:3,他引:16       下载免费PDF全文
由于风浪对浅水湖泊底泥的强烈扰动作用,底泥再悬浮的生态效应研究成为目前国际研究热点之一.但方法的缺乏极大地限制了有关底泥再悬浮环境效应的深入研究.本研究应用一种新的沉积物再悬浮装置,模拟了太湖南部长兜港水域不同风浪影响下悬浮物的垂向分布,获得水柱总悬浮物量(T)与扰动频率(n)的定量关系:T=19.77×exp(n/2.61)-71.7.结合现场实测风情下的水柱总悬浮物量,建立了室内水动力条件、水柱总悬浮物量和现场风情的定量关系.研究2004年10月至2005年10月太湖全年代表性小风、中风及大风与再悬浮装置的扰动频率对应关系,估算了小风、中风和大风常规风情引起的总悬浮物量分别为159、230、425 g/m2.结果表明,模拟获得的太湖悬浮物垂向分布规律与现场状况较为接近,是目前较为适用的浅水水体沉积物再悬浮模拟方法.  相似文献   

9.
采用三维荧光光谱-平行因子法(EEMs-PARAFAC)分析太湖五里湖水体悬浮物中水溶性有机质(WSOM)的荧光光谱特征,研究其组分类型、分布规律以及来源,进一步探讨悬浮物中水溶性有机氮和无机氮含量与WSOM荧光组分之间的关系.结果表明,悬浮物中WSOM荧光组分主要由2个类腐殖质(C1、C2)和1个类色氨酸类蛋白质(C3)组成.总荧光强度在57.56~200.01 R.U./g之间,平均为115.42 R.U./g,其中C1、C2、C3的相对比例分别为35.55%、34.05%和30.40%;空间上由西向东逐渐增强,东五里湖高于西五里湖,沿岸区高于湖心区.荧光指数和生物源指数变化范围分别在1.48~2.34和0.65~0.87之间,反映了悬浮物中WSOM主要来源于微生物、藻类的自生生物源.多元回归统计分析结果表明,悬浮物WSOM与氮元素的迁移转化密切相关,且有机氮与WSOM荧光组分的相关系数大于无机氮.  相似文献   

10.
浅水湖泊沉积物磷释放的波浪水槽试验研究   总被引:15,自引:1,他引:15  
为探索浅水湖泊水动力扰动作用对沉积物内源营养盐释放的规律,采用波浪水槽试验研究了波浪扰动对太湖和巢湖沉积物悬浮和磷释放的作用.试验结果显示在强波浪扰动下,底泥大规模悬浮,使得水体中悬浮固体(SS)、总磷(TP)和溶解性总磷(DTP)含量显著升高,太湖和巢湖底泥水槽试验中上覆水体TP含量分别升高了6倍和3倍,DTP分别升高了1倍和70%,太湖底泥试验中溶解性活性磷(SRP)含量亦升高了25%.掀沙过程中,不但表层底泥间隙水中的溶解性磷释放到上覆水体当中,沉积物颗粒所吸附的磷也大量转化为SRP而解吸释放.然而,强波浪掀沙一段时间后,溶解态磷的释放逐渐受到限制.随着波浪扰动作用的持续,悬浮物的中值粒径减小,细颗粒组分的百分含量明显增加,使得悬浮物对溶解态磷的吸附能力增强;波浪扰动显著提高了水体的溶解氧浓度,也会促进水体铁锰物质的氧化,增大其对磷酸根离子的吸附能力.这些变化可能是波浪掀沙后期限制水体SRP浓度进一步升高的主要原因.太湖底泥波浪水槽试验的结果与太湖梅梁湾中心区域常见风浪扰动下底泥的悬浮起动情况相吻合,底泥起动的临界切应力也基本相同,强波浪掀沙的切应力条件及水体SS,TP及SRP浓度变化的特点也一致,表明本实验的结果接近太湖的实际状况.本研究说明太湖的水动力扰动能显著提高水体TP及SRP浓度,大波掀沙初期对底泥磷释放的影响最大,后期的影响强度则有所下降.  相似文献   

11.
It was indicated in this study that there were negative relations between the concentrations of suspended solid (SS) and transparency according to the analysis of measured data of Lake Taihu. Their relations in pervious studies were reviewed, which showed that the changes of transparency in Lake Taihu could be reflected by simulating suspended solid concentration (SSC). Measured data showed that the changes of SSC with wind speed were similar at different water depths. SSC increased with the increasing of wind speed. Both wave and lake current of Lake Taihu had positive relations with SSC. However, wave was the main factor affecting sediment suspension, while flow took the second place. In this study, a numerical model coupling lake current, wave and SSC of Lake Taihu was developed. In the SS model, the combined effects of wave and current were included. The amounts of suspended and deposited sediments near the lake bed surface layer were treated separately. The stochastic characteristics of turbulent flow pulsation near lake beds were also considered, and the start-up conditions of sediment suspension were introduced to the model. The model elucidated the mutual exchange processes between sediment particles in SS and active sediments within and on the bed surface layer. Simulated results showed that lake current had relatively significant effects on the SSC at littoral areas of Lake Taihu, while SSC at the central area of the lake was mainly influenced by wave. The changes of transparency with SSC were simulated for Lake Taihu using this model. Calculated results were validated by measured data with good fitness, which indicated that the model is basically suitable for the simulation and prediction of transparency of Lake Taihu.  相似文献   

12.
It was indicated in this study that there were negative relations between the concentrations of suspended solid (SS) and transparency according to the analysis of measured data of Lake Taihu. Their relations in pervious studies were reviewed, which showed that the changes of transparency in Lake Taihu could be reflected by simulating suspended solid concentration (SSC). Measured data showed that the changes of SSC with wind speed were similar at different water depths. SSC increased with the increasing of wind speed. Both wave and lake current of Lake Taihu had positive relations with SSC. However, wave was the main factor affecting sediment suspension, while flow took the second place. In this study, a numerical model coupling lake current, wave and SSC of Lake Taihu was developed. In the SS model, the combined effects of wave and current were included. The amounts of suspended and deposited sediments near the lake bed surface layer were treated separately. The stochastic characteristics of turbulent flow pulsation near lake beds were also considered, and the start-up conditions of sediment suspension were introduced to the model. The model elucidated the mutual exchange processes between sediment particles in SS and active sediments within and on the bed surface layer. Simulated results showed that lake current had relatively significant effects on the SSC at littoral areas of Lake Taihu, while SSC at the central area of the lake was mainly influenced by wave. The changes of transparency with SSC were simulated for Lake Taihu using this model. Calculated results were validated by measured data with good fitness, which indicated that the model is basically suitable for the simulation and prediction of transparency of Lake Taihu.  相似文献   

13.
不同水动力扰动下太湖沉积物的悬浮特征   总被引:8,自引:2,他引:8  
利用2002年7月及2003年4月分别在太湖乌龟山和梅梁湾的水动力观测资料,计算了波浪和湖流产生的湖底切应力,分析了二者对太湖沉积物悬浮的不同贡献.结果发现,在小扰动情况下,流切应力大于波切应力,但不能引起沉积物的悬浮;在强扰动情况下,底流对沉积物悬浮的影响可以忽略,且扰动越强,其作用越小,而波浪的影响却愈加突出;在中等扰动下,二者的相互作用产生沉积物的悬浮,但波浪的作用较为显著.该结论能为计算太湖水体悬浮物浓度和动态内源释放提供重要的参考依据.  相似文献   

14.
波浪作用下太湖底泥试验及航道回淤分析   总被引:4,自引:1,他引:4  
波浪作用下泥沙的起动和输移研究对航道回淤分析具有重要意义.以往这类研究主要针对海岸地区的非粘性沙,而对于单纯波浪或以波浪为主要动力的粘性泥沙运动,特别是湖区底泥的研究相对较少.本文通过波浪水槽试验对太湖底泥的起动和输移进行了研究,并提出波浪动力下含沙量经验公式,由此对太湖地区某具体工程的航道回淤进行分析计算.该成果对研究波浪作用下淤泥的输移及太湖地区类似的航道回淤问题具有借鉴意义.  相似文献   

15.
分季节的太湖悬浮物遥感估测模型研究   总被引:6,自引:0,他引:6       下载免费PDF全文
根据1996-2002年无锡太湖监测站的水质资料分析,太湖悬浮物具有季节性特征,因而分季节的悬浮物估测模型比单一的模型可能更加适合用来估测太湖全年的悬浮物浓度.在分析太湖水体光谱特征的基础上,根据太湖悬浮物的季节性分布特征,使用春夏秋冬四季的Landsat TM/ETM图像和准同步的水质采样数据,建立了太湖分季节的悬浮物估算模型.结果表明:估测因子(B2 B3)/(B2/B3)在春、秋、冬三季都能很好地估测出悬浮物的浓度(R2>0.52).夏季由于叶绿素的干扰性较大,悬浮物的估测效果不理想.冬季的估测效果最好(R2=0.81),模型为lnSS=14.656×(B2 B3)/(B2/B3) 1.661,其中,ln SS表示悬浮物取自然对数后的值,B2、B3为TM/ETM图像经过6S大气校正、3×3低通滤波后第2、3波段的反射率值.  相似文献   

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1 INTRODUCTION Large amounts of nutrients and contaminants such as trace metals are transported into large lakes frominflow rivers and then absorbed onto or associated with fine-grained sediment particles (Sheng and Lick,1979). The nutrients and contamina…  相似文献   

17.
Influence of wave on sediment resuspension and nutrients release from sediments, collected from Lake Taihu and Lake Chaohu, was studied in flume experiments. Under strong-wave conditions, concentrations of suspended solids (SS), total phosphorus (TP) and dissolved total phosphorus (DTP) in overlying water were increased significantly following the sediments re-suspension. During the experiments on sediments of Lake Taihu and Lake Chaohu, TP concentrations increased 6 times and 3 times, and DTP concentration increased 100% and 70% more than it in presuspension, respectively. Concentration of soluble reactive phosphorus (SRP) of experiment on sediment of Lake Taihu increased 25%. During the massive sediment suspension, the dissolved phosphorus in pore water and much of the phosphorus adsorbed by the sediment particles were released into overlying water. The phenomena in this wave flume experiment are quite similar to the situation observed in situ of Lake Taihu. The critical wave stresses of sediment re-suspension are nearly equal. The change of concentrations of SS, TP, and SRP was the same as that in situ situation. This study showed that concentrations of TP and SRP in lake water could be increased significantly by wave disturbance. Phosphorus release was significantly enhanced by wave disturbance at the beginning of massive sediment re-suspension, but decreased later.  相似文献   

18.
Influence of wave on sediment resuspension and nutrients release from sediments, collected from Lake Taihu and Lake Chaohu, was studied in flume experiments. Under strong-wave conditions, concentrations of suspended solids (SS), total phosphorus (TP) and dissolved total phosphorus (DTP) in overlying water were increased significantly following the sediments re-suspension. During the experiments on sediments of Lake Taihu and Lake Chaohu, TP concentrations increased 6 times and 3 times, and DTP concentration increased 100% and 70% more than it in presuspension, respectively. Concentration of soluble reactive phosphorus (SRP) of experiment on sediment of Lake Taihu increased 25%. During the massive sediment suspension, the dissolved phosphorus in pore water and much of the phosphorus adsorbed by the sediment particles were released into overlying water. The phenomena in this wave flume experiment are quite similar to the situation observed in situ of Lake Taihu. The critical wave stresses of sediment re-suspension are nearly equal. The change of concentrations of SS, TP, and SRP was the same as that in situ situation. This study showed that concentrations of TP and SRP in lake water could be increased significantly by wave disturbance. Phosphorus release was significantly enhanced by wave disturbance at the beginning of massive sediment re-suspension, but decreased later.  相似文献   

19.
The internal sediment release is a key factor controlling eutrophication processes in large, shallow lakes. Sediment resuspension is associated with the wave and current induced shear stress in large, shallow lakes. The current study investigated the wind field impacts on sediment resuspension from the bottom at Meiliang Bay of large, shallow Lake Taihu. The impacts of the wind field on the wave, current, and wave-current combined shear stresses were calculated. The critical wind speed range was 4–6?m/s after which wave and current shear stress started to increase abruptly, and onshore wind directions were found to be mainly responsible for greater shear stress at the bottom of Lake Taihu. A second order polynomial fitting correlation was found between wave (R2 0.4756) and current (R2 0.4466) shear stresses with wind speed. Wave shear stress accounted for 92.5% of the total shear stress at Meiliang Bay. The critical wave shear stress and critical total shear stress were 0.13?N/m2 for sediment resuspension whereas the current shear stress was 0.019?N/m2 after which suspended sediment concentrations (SSC) increased abruptly. A second order polynomial fitting correlation was found between wave (R2 0.739), current (R2 0.6264), and total shear stress (R2 0.7394) with SSC concentrations at Meiliang Bay of Lake Taihu. The sediment resuspension rate was 120 to 738?g/m2/d during 4–6?m/s onshore winds while offshore winds contributed ≥ 200?g/m2/d. The study results reveal the driving mechanism for understanding the role of the wind field in sediment resuspension while considering wind speed and direction as control parameters to define wave and current shear stresses.  相似文献   

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