东海混浊海域悬沙浓度的三维数值模拟及与观测的比较

借助ECOMSED模式进行了东海混浊水海域三维悬浮泥沙输运的数值模拟,其中水动力模拟中考虑了潮汐,海流（包括黑潮,长江径流等）及风场的作用,输运模型中考虑了粘性泥沙的絮凝、粘性和非粘性泥沙的再悬浮等过程。另外,在沉积输运模式中,增加了波浪的作用,使沉积输运模拟更完善,并与2006年8月份在长江口外海域获得的走航断面及定...     

山东半岛沿岸海域悬浮体时空分布及形成机制分析

依据2015年GOCI(geostationary ocean color imager)卫星影像反演的悬浮体浓度数据,分析了山东半岛沿岸海域表层悬浮体质量浓度和锋面月变化特征,揭示该海域悬浮体的分布特征和扩散格局,并结合风速、波高以及海表温度数据,对其控制因素进行初步探讨。结果显示:研究区内悬浮体质量浓度整体表现为冬季最高,春秋次之,夏季最低的分布特征;悬浮体扩散过程可以划分为4个阶段,冬季稳定外输,春季向岸退缩,夏季近岸贮存,秋季向外扩散。此外,山东半岛近岸存在一条悬浮体质量浓度高于10 mg/L的浑浊带,该浑浊带同样表现出季节变化,它在秋季开始形成,其悬浮体含量、幅宽及延伸范围在冬季达到最大,春季减弱,夏季消失。研究认为山东半岛沿岸海域的表层悬浮体来源主要是海底沉积物的再悬浮。风场、海浪以及沿岸流的强弱变化对悬浮体分布和输运的季节变化有重要的控制作用:风场和海浪影响海水混合搅拌强度,改变海底沉积物再悬浮作用的临界深度,进而影响表层海水悬浮体浓度,致使悬浮体浓度与风浪的月际变化趋势基本一致;沿岸流携带高浓度悬浮体沿山东半岛输运形成沿岸浑浊带,沿岸流的强度变化直接控制浑浊带的季节变化。     

黄河入海物质输运通道

渤海水体浊度的分布及其季节变化反映了悬浮物质的分布、输运及其季节特征。本文利用2012—2016年渤黄海8个航次现场观测的水体温度、浊度数据,并结合CCMP(Cross—CalibratedMulti—Platform)风场数据、ROMS(RegionalOceanModelSystem)海流数值模拟结果,分析了渤海海域水体浊度季节分布特征。水体浊度的大小与风速的季节变化密切相关,冬季,黄河口及附近海域的浊度值最高,离岸31km到56km处浊度值从180NTU迅速下降至54.3NTU,而其他季节的浊度较低;渤海全年20m以深海域再悬浮较弱,以水平扩展为主。进而甄别了黄河口附近高浊度水体向渤黄海输运的两条路径,分别为:冬夏季均存在的沿渤中浅滩西侧通道向渤海北部扩展和冬季存在的沿莱州湾湾口向渤海海峡南部及北黄海输运,该两条路径主要由环流场控制。     

辽东半岛东岸近海泥区悬沙浓度的时空分布及控制因素分析

鸭绿江作为典型的中小型河流,细颗粒沉积物从鸭绿江流域到辽东半岛东岸近海泥区的源汇过程有着独特的机制,而遥感解译是了解入海沉积物在河口-陆架输运过程和机制的有效手段之一。因此,本文通过在辽东半岛东岸海域进行了现场悬沙浓度测量,并与GOCI影像建立关系,反演了该地区2011年4月至2017年3月间的表层悬沙浓度,从而揭示了该海域表层悬沙浓度的时空特征,分析了潮流、大风天气和洪水对悬沙浓度变化的影响,在此基础上探讨了研究区的悬沙浓度输运格局。结果显示,研究区表层悬沙浓度空间差异大,河口附近是悬沙浓度高值区,可达500 g/m3以上,其他区域则悬沙浓度多小于20 g/m3。另外,研究区表层悬沙浓度枯季高,洪季低,有着显著的季节性变化。进一步分析表明,枯季大风天气引起的风浪作用增强,是导致表层悬沙浓度增高的主要原因;洪季虽然悬沙浓度较低,但流域洪水期间的悬沙浓度显著增加。此外,作为典型的中小型源-汇传输体系,沉积物从鸭绿江到辽东半岛东岸近海泥区总体上仍遵循"夏储冬输"的输运机制。     

基于波-流耦合模型的珠江口悬浮泥沙数值模拟

为研究珠江口悬浮泥沙输运动力机制,本文发展了一套三维波、流、泥沙耦合数值模型。模型结果与观测数据吻合较好,统计显示模型获得良好的评分分值。利用数值模拟研究了不同强迫（径流,波浪和风）对珠江口中悬浮泥沙的影响。模型结果表明,河口重力环流对珠江口最大浑浊带的发展起着重要作用,特别是在小潮期间。另外,径流的增加可导致泥沙向海输运。底部的悬浮泥沙浓度随着波浪底部轨迹速度和波高的增大而增加。由于西滩水深较浅,波浪对西滩悬浮泥沙的影响大于东槽。西南风引起的波浪对悬沙的影响大于东北风引起的波浪的影响,而东北风致流对悬沙的影响略大于对西南风致流的影响。在其他条件相同情况下,稳定的西南风比稳定的东北风更有利于伶仃洋悬浮泥沙浓度的增加;在稳定的西南风下,伶仃洋平均悬浮泥沙浓度约为稳定东北风下的1.1倍。     

Contribution of waves and currents to sediment resuspension in the Yellow River Delta

The objective of this study was to investigate that the effects of different hydrodynamic conditions on sediment resuspension on a tidal mudflat in the Yellow River Estuary. A field experiment was conducted on an intertidal flat of the Yellow River Delta, China. The sediment resuspension concentrations and hydrodynamic conditions were obtained in the field from September 2–7, 2013. The resuspended sediment concentrations induced by wave loading were compared with those induced by coupled wave–current actions in Yellow River Delta. The results were as follows: (1) when the wave height was higher than 10?cm and the shear stress induced by the waves was greater than the critical stress of the seabed sediments, the surface seabed was eroded and sediment was resuspended. In addition, 60% of the significant wave heights were larger than 10?cm on the intertidal flat of the Yellow River Delta. (2) The contribution of waves to sediment resuspension was greater than 30% when the significant wave height is higher than 10?cm, and the average contribution of waves to sediment resuspension was 51%. The mechanism of wave-induced sediment resuspension and processes of sediment resuspension were described in this paper.     

Anomalous current recorded at lower low water off the Changjiang River mouth,China

A hydrographic-sedimentological investigation was conducted in May 2001, aimed at assessing dynamic sedimentation patterns near and off the Changjiang River mouth, East China Sea. Current speed/direction, suspended sediment concentration (SSC), and turbidity were measured at eight nearshore and offshore sites, spanning a distance of ca. 150 km. The results identified a high-speed current ranging from 0.9 to 1.6 m/s at lower low water in the front of the turbidity maximum zone. This anomalous current, lasting about 4 h, was the fastest recorded over two semi-diurnal tidal cycles. Simultaneous measurements showed a high SSC (0.5 g/l) and high turbidity (>230 ppm) near the seafloor. This phenomenon would help explain periodic enhancement of sediment resuspension in the area, and an associated southward transport route from the Changjiang River mouth.     

基于ADCP反演渤海湾悬浮体浓度年变化

基于座底ADCP实测回波强度信号,结合短期实测悬浮体质量浓度,反演长时间序列悬浮体质量浓度,定量分析了渤海湾近一年悬浮体质量浓度变化特征及其影响因素。结果表明:受风浪影响,该区悬浮体质量浓度具有明显季节性变化特征,风浪作用强烈的季节其悬浮体浓度表现为相对高值。悬浮体净输运同样具明显季节性变化,秋冬强风浪作用下,悬浮体的净输运量明显增加;而在不同季节,月净输运方向具有不同的主输运方向。悬浮体质量浓度日变化受潮流控制明显,长周期变化则主要与风场的变化有关。潮流涨急过程与风致大浪过程均可引起沉积物再悬浮,导致悬浮体浓度明显增高。     

台风事件对东中国海悬沙浓度时空演变的影响分析

东海大陆架常受台风侵扰, 强风浪在破坏水体结构的同时引起大量泥沙再悬浮。台风是影响东海表层悬沙浓度(suspended sediment concentration, SSC)的主要动力之一。本文将台风类型分为登陆和非登陆两大类共八种。基于GOCI (geostationary ocean color imager)遥感数据统计分析了2017~2020年9个不同类型台风事件对表层悬沙浓度时空分布的影响。结果表明, 近海活动型和远海活动型台风使SSC显著增高了150%~200%; 随着风速减小, SSC逐渐下降, 但需要3~4 d才能恢复至台风之前的SSC。风速变化与SSC变化率的相关性高达0.86。近海及远海活动型台风影响研究区域的风向为偏北风, 该类型台风使秋季SSC等值线向外海延伸, 出现舌状分布特点; 而登陆型台风影响研究区域的风向前期为偏北风, 后期为偏南风, 该类型台风使SSC等值线呈基本平行向外海移动较短距离, 但不出现向外海延伸的舌状分布。近海及远海活动型台风事件使SSC分布迅速向气候态平均天气下的冬季输运类型转变, 其中近海活动型台风对SSC分布的影响比远海活动型更显著。登陆型台风对研究区域SSC跨陆架方向分布的影响比远海活动型台风更小。     

波浪、潮流和风暴潮耦合模式及悬沙输移规律的研究

近年来，由于河口、海岸地区的泥沙运动与港口、航道以及海岸的冲淤有着直接的关系，对一些海岸建筑物比如防波堤、护岸工程等造成一定的威胁，甚至于使其完全丧失使用价值，造成巨大的损失。为此人们越来越重视对这一问题的研究。本文为估计岸滩的冲淤变化和了解岸滩的演变规律，对影响泥沙运动的海洋动力要素进行了研究。 为研究悬沙的输移规律，建立了一个由两部分组成的二维悬沙模型系统：①水动力模式。建立了一个综合多因素的二维波浪、潮汐和风暴潮耦合模式，以此来研究波、潮、风暴潮间的相互作用，并为泥沙计算提供流速场。②二维悬沙模式。运用得出的流场来研究悬沙的输移扩散规律。其中所采用的波浪模式是将流对波浪场的影响同时加以考虑的耦合数学模型，将流速加入波能方程，并考虑由于水面的升降而产生的不定常水深对波浪场的影响，再将波浪场对流场的影响通过辐射应力、考虑波浪影响的底应力以及依赖波龄的表面风应力耦合到流场中，从而建立了一个综合多种因素的波浪、潮汐、风暴潮联合作用下的二维悬沙模型系统。并在此模型系统的基础上，对黄河口泥沙的输移问题作了探讨，为今后的防堤、护岸工程提供依据。     

江苏近岸海域悬沙浓度的时空分布特征

2006—2007年间的四个季节在江苏近岸海域69个站位采集水样,获取悬沙浓度。通过对TM遥感数据反演,获取该海域四季大面悬沙浓度,并与调查的实测悬沙浓度进行对比。结果显示,大面调查的非同步数据基本可正确反映大区域悬沙浓度的季节与空间分布趋势。悬沙浓度等值线由高至低、由陆向海分布,底层浓度约为表层的2—3倍;废黄河口和长江口外海域为悬沙浓度高值区,而海州湾为低值分布区,东南部陆架区受台湾暖流影响出现低值中心。冬季整个海域悬沙浓度均较高,其次为春季,夏季最低;废黄河口海域的高值中心在不同季节分布位置有所移动。海底沉积物的再悬浮是苏北近岸悬沙最主要的来源,河流输沙量的季节变化是影响长江口海域悬沙浓度变化的关键因子。相关分析结果表明,潮流为影响悬沙浓度分布的主要控制因子;季风、风暴潮和风浪虽对悬沙的分布具有一定的影响,但冬季的低温环境是形成该季节整个海域悬沙浓度显著偏高的重要因素。     

青岛近海悬沙输运的三维数值模拟

研究近海海域水流、悬沙运动规律,运用基于COHERENS发展的水动力悬沙模型COHERENS-SED,结合当地一般波浪条件,模拟了青岛近海悬浮泥沙输运情况,并验证及分析了水动力环境及悬沙输运的模拟结果。结果表明：在波流合作用下,近岸掀沙明显,大潮期间该海域近岸悬沙浓度值最高可达50mg／L。     

基于遥感反演的莱州湾悬沙分布及其沉积动力分析

选用1986-2004年不同时期的LandsatTM/ETM+影像,利用2004年黄河口附近实测数据推导的表层悬浮泥沙浓度反演模型,结合水文气象资料、多年水深数据和极端天气数模结果,研究了莱州湾西南近岸海域表层悬浮泥沙分布特征,结果表明,受黄河丰枯水期的影响,莱州湾西南部海域悬浮泥沙高浓度区主要分布于黄河口附近海域和西南沿岸,其枯水期的覆盖范围一般大于丰水期的。受潮流高流速场控制,黄河口外悬沙浓度高值区与海底泥沙堆积区对应较好,泥沙主要来源于陆源输沙和泥沙再悬浮;在西南近岸浅海区悬沙浓度高值区主要形成于泥沙的再悬浮,在近岸出现轻微冲刷。风等其他海洋动力因素,一般情况下对悬浮泥沙扩散的程度和范围具有一定的影响作用,但悬沙受潮流场影响而形成的总体扩散趋势未发生改变;极端条件下,风暴潮流使莱州湾西南部近岸浅海区的悬浮泥沙浓度显著增加。     

南黄海辐射沙洲附近海域悬浮体的研究

对2003年春季(3—4月)和秋季(9月)南黄海辐射沙洲附近海域的悬浮体样品进行了空间分布特征、有机无机组成、粒度特征及其季节变化分析。结果表明:(1)2003年春季研究区内悬浮体浓度要普遍高于秋季的悬浮体浓度。悬浮体浓度最高值区位于长江口-老黄河口之间的近岸区。陆源物质为主的无机组分是悬浮体的主体成分,特别是在近岸浅水区和接近海底的底层水中尤为突出;(2)研究区海水中的悬浮体主要来源于辐射沙脊区(老黄河-长江复合三角洲)沉积物再悬浮;(3)悬浮体分布是风浪、潮流及沿岸流等多种因素综合作用的结果,而风浪和潮流是影响本区悬浮体分布的主要因素,巨大的风浪和强大的潮流造成辐射沙洲海底的沉积物再悬浮、搬运和再沉积,并在苏北沿岸流的作用下向沙洲外缘输运。     

黄河三角洲海底土波致再悬浮研究

在现代黄河三角洲采集土样,制备室内水槽试验的底床,施加波浪作用,观测波致悬沙含量的变化规律,分析不同波高、作用时间对单位面积底床再悬浮量的影响,及波浪停止作用后悬浮泥沙的静水沉降规律。研究发现,在水深一定条件下底床再悬浮量呈现随波高增大而增大的特性,两者线性拟合的相关性很好;在一定波高的波浪连续作用下,约5 000~6 000个波周期底床再悬浮过程完成;在波浪作用初始阶段底层悬沙含量与中上层的相差很大,悬沙含量垂线结构呈斜线型,稳定阶段的悬沙浓度垂向结构呈准直线型,底层与表层含沙量比值为0.98~1.25,整个水层含量分布均匀;静水沉降过程中当悬沙含量大于1 g/dm3,悬沙含量(SSC)呈现出随时间指数衰减的规律,悬沙浓度与沉降通量呈线性关系。研究结果对认识黄河水下三角洲泥沙运移规律具有一定的科学意义。     

A numerical study of transport dynamics and seasonal variability of the Yellow River sediment in the Bohai and Yellow seas

A sediment numerical model was embedded into a wave-tide-circulation coupled model to simulate the transport processes of the Yellow River-derived sediment considering the wave-induced vertical mixing (Bv) and the wave-current coupled bottom shear stress (BSS). Numerical results show that the main stream of the Yellow River-derived sediment moves first eastward off the northern Shandong Peninsula and then southward into the South Yellow Sea all year round. In spring, the sediment moves northeastward in the Bohai Sea. In summer, there is a northeastward branch of sediment in the Bohai Sea off the west coast of the Liaodong Peninsula, while the main part goes eastward to the Yellow Sea. The Yellow River-derived sediment transport from the Bohai Sea to the North Yellow Sea across the Bohai Strait is mainly limited to the top 10 m, and with a maximum centered at 37.9°N in summer. The transport from the North Yellow Sea to the South Yellow Sea across the transect of 37°N is mainly in the 0–30 m layer with a maximum around 123.7°E in autumn. The simulated Yellow River-discharged sediment deposits along the Shandong Peninsula and between 20 and 30 m isobaths in the Yellow Sea, which is consistent with observation. If surface waves are not considered in the model, the sediment deposits westward to the nearshore area in the South Yellow Sea. The sediment would deposit further southward in the numerical experiment results without wind influence. In the numerical experiment of no tide, there is hardly any sediment deposited on the Yellow Sea floor, while in the Bohai Sea most of the sediment is transported southward and northwestward around the river mouth instead of eastward as in the Control Run, indicating the tides play a key role in forming the deposition pattern.     

1988-2002年黄海和渤海风浪后报

本文对黄海和渤海风浪开展长期后报实验,时间范围覆盖1988至2002年,并分析相应的区域波候特征。首先,模式输出的月平均有效波高和卫星数据比对一致。其次,我们讨论了气候态月平均有效波高和平均波周期的时空分布特征。有效波高和平均波周期的气候态空间分布都呈现出西北-东南、或由近岸向深水区增加的趋势,这种空间的分布特征和局地的风强迫和水深密切相关。同时,海浪参数的季节变化也较显著。进一步,我们统计分析了风场和有效波高的极值,给出并揭示了黄海和渤海多年一遇有效波高的空间结构,并讨论了有效波高极值和风强迫极值之间的联系。     

Distribution and its mechanism of suspended particulate matters in the southern Huanghai Sea and the East China Sea in summer

Water temperature,turbidity,chlorophyll-a and suspended sediment concentration (SSC) were investigated at 61 stations of eight sections in the southern Huanghai Sea (HS) and the East China Sea (ECS) during the summer (28 June to 15 July) of 2006.The horizontal distribution of suspended parti culate matter (SPM) displayed a high concentration inshore and a low value offshore.The maximum value can reach 10.4 mg/dm 3,which can be found at the Changjiang River mouth.For the same site,the SSC was generally higher at the bottom than on the surface.In the vertical direction,distribution characteristics of turbidity can be divided into two types:in the southern HS high values at the bottom while low values on the surface,and in the ECS high values inshore with low values offshore.The thermocline in the HS and the Taiwan Warm Current in the ECS could be important factors preventing the SPM from diffusing upward and seaward.Even the typhoon Ewiniar was not able to work on the major sediment transport under the thermocline during the observation.     

1988—2009年中国海波候、风候统计分析

利用高精度、高时空分辨率、长时间序列的CCMP(Cross-Calibrated,Multi-Platform)风场,驱动国际先进的第三代海浪模式WAVEWATCH-Ⅲ(WW3),得到中国海1988年1月～2009年12月的海浪场。对中国海的波候(风候)进行精细化的统计分析,分析了海表风场和浪场的季节特征、极值风速与极值波高、风力等级频率和浪级频率、海表风速和波高的逐年变化趋势,结果显示:(1)中国海的海浪场与海表风场具有较好的一致性,尤其是在DJF(December,January,February)期间;海表风速和波高在MAM(March,April,May)期间为全年最低,在DJF期间达到全年最大;MAM和JJA(June,July,August)期间,中国海大部分海域的波周期在3～5.5s,SON(September,October,November)和DJF期间为4.5～6.5s。(2)中国海极值风速、极值波高的大值区分布于渤海中部海域、琉球群岛附近海域和台湾以东广阔洋面、台湾海峡、东沙群岛附近海域、北部湾海域、中沙群岛南部海域。(3)吕宋海峡在MAM、SON、DJF期间均为6级以上大风和4m以上大浪的相对高频海域,JJA期间,6级以上大风的高频海域位于中国南半岛东南部海域,4m以上大浪主要出现在10°N以北。(4)在近22a期间,中国海大部分海域的海表风速、有效波高呈显著性逐年线性递增趋势,风速递增趋势约0.06～0.15m.s-1.a-1,波高递增趋势约0.005～0.03m.a-1。     

Simulation of Suspended Sediment in the Yellow and East China Seas

Described is an initial attempt to simulate the suspended sediment dynamics relating to tidal and wave forcing during summertime in June 1980 and August 1981 for the Yellow and East China Seas continental shelf. The cohesive/non-cohesive sediment resuspension and movement generated by the interaction between current and wave are modeled by use of ECOMSED and WAM Cycle 4. Model results are compared with observations in US-China Marine Sedimentation Dynamics Program performed for 1980-81 at off the Changiiang estuary. The main features of simulations show that suspended sediment concentrations during the summer decreased markedly offshore as observed during the simulation periods. As for some discrepancies for the mouth of the estuary with high river discharges, i.e., the Changjiang River, the model did not properly reproduce the over-mixing situation in the summer; thus distinct vertical concentration variation in this local region is not agreeable with observation. However, general dispersal patterns of suspended sediment movement seem to be agreeably reproduced for the nearshore shallow region. Some of the procedures of simulation and results are presented and discussed.