洋浦湾南浅滩-深槽-拦门沙近40年冲淤变化分析

本文根据1965、1984、1999和2005的海图对比分析, 探讨了洋浦湾深槽、南浅滩以及口外拦门沙的冲淤变化, 得出: 1)1965—1984年之间, 南浅滩呈淤涨之势, 其西南部最大淤涨距离可达640m; 1984—1999年南浅滩出现了侵蚀, 这主要是由于洋浦湾波浪以及沿岸流的作用引起的; 1999—2005年, 靠近口门附近的南浅滩出现淤涨现象, 主要是由于洋浦湾口门附近水动力的影响作用; 但是目前整体基本上处于稳定的阶段。2)洋浦深槽段呈现出不同程度的西边坡淤涨, 东边坡侵蚀后退, 深泓断面缩窄、淤浅及东偏的趋势, 特别是剖面5的变化比较复杂,值得关注。3)口外拦门沙近几十年来呈现出不同的时空冲淤变化, 但是以淤积为主, 1965—2005年拦门沙总的淤积厚度达到1m左右, 但随着泥沙补给的减少, 这种淤积趋势也随着减少。     

近50 a来辽河口水下三角洲演变特征研究

本文基于近50 a来的辽河口海域的水下地形资料,采用GIS技术手段研究了辽河口水下三角洲的演变特征。研究结果表明:近50 a来辽河水下三角洲外缘(蛤蜊岗子滩西缘和南缘、西滩西缘和南缘)出现较大幅度的侵蚀后退;蛤蜊岗子滩东缘淤积外移,南部滩尾东部有北移东偏趋势;近岸浅滩由淤涨变为基本稳定,局部有所侵蚀后退;受蛤蜊岗子滩向东淤进的影响,蛤蜊岗子滩东侧深槽有所缩窄;蛤蜊岗子滩和西滩之间深槽水域出现拓宽变浅的变化趋势。流域来水来沙减少是近年来辽河口水下三角洲外缘侵蚀后退的主要原因,外缘侵蚀泥沙在波流作用下向河口搬运是蛤蜊岗子滩东侧淤积、深槽缩窄的主要原因,近岸边滩人工围垦对水下三角洲演变的影响值得关注。     

乳山湾泥沙运移趋势及蚀淤分析

采用单宽输沙、沿岸输沙、海图对比及钻孔分析等方法,研究了乳山湾内泥沙运移趋势及蚀淤量变化两方面问题,蚀淤分析将乳山湾划分为:东汊、西汊、潮流通道和口门4部分进行讨论。研究认为乳山湾以河流来沙为主,湾内泥沙主要被落潮流带出湾外,在口门附近沉降形成落潮流三角洲,湾外两侧岸段破波带泥沙主要向口门方向运移,而悬移质泥沙主要被涨潮流带向湾顶。淤积区域集中在东西两汊及口门附近,潮流通道以侵蚀为主,东汊淤积速率为0.4~13.2 cm/a,口门附近淤积速率为6~20 cm/a,潮流通道侵蚀速率在5.7~23 cm/a之间。     

黄茅海河口湾现代动力地貌体系和冲淤过程分析

1980—1993年对黄茅海河口湾进行沉积物采样和水流测定及水深测量。根据水动力和地形条件，冲淤分析及Mclaren模型研究河口湾的动力地貌体系、冲淤特征和现代沉积物运移。结果表明：（1）水下地形主要为下泄流或上溯流控制的“深槽－槽沟－浅滩－湾口”的动力地貌体系，反映了河口湾“东进西出”的水流格局；（2）整个河口湾以淤积为主，只有崖门深槽有较明显的优势冲刷特征，并随着崖门深槽向海推移和河口湾“东进西出”水动力作用，黄茅海落潮三角洲相应向西南进积；（3）应用Mclaren模型揭示了黄茅海河口湾现代沉积物运移规律，同样反映了河口湾具有“东进西出”的运移趋势。     

华南海岸沙坝瀉湖型潮汐汊道口门地貌演变

华南海岸沙坝Ｘｉ湖型潮汐汊道主要分布在小潮差岬湾海岸段。汊道口门基本地貌单元有口门深槽、落潮三角洲、涨潮三角洲、内湾沙嘴等。其形态特征与海岸动力及泥沙条件有关。汊道口门迁移、落潮主水道迁移、冲流坝和水道边缘坝向岸迁移和并岸，是汊道口门地貌演变的主要模式并具周期性特点。Ｘｉ湖港湾大规模围垦堵海或注入港湾的河流改道直接入海，这些人类活动可能导致汊道口门急剧变化和航行条件恶化而必须进行整治。     

华南海岸沙坝瀉湖型潮汐汊道口门地貌演变

华南海岸沙坝湖型潮汐汊道主要分布在小潮差岬湾海岸段。汊道口门基本地貌单元有口门深槽、落潮三角洲、涨潮三角洲、内弯沙嘴等，其形态特征与海岸动力及泥沙条件有关。汊道口门迁移、落潮主水道迁移、冲流坝和水道边缘坝向岸迁移和并岸，是汊道口门地貌演变的主要模式并具周期性特点。　湖港湾大规模围垦堵海或注入港湾的河流改道直接入海，这些人类活动可能导致汊道口门急剧变化和航行条件恶化而必须进行整治。     

泉州湾泥沙运移与冲淤变化

运用"粒径趋势分析"方法研究泉州湾泥沙净输运趋势,借助210Pb测年法测定湾内北水道的沉积速率,并通过海图对比计算海湾冲淤变化.结果表明,泉州湾总体处于淤积之中,但湾内冲淤分布不平衡:北水道淤积程度重,其中上游是湾内的现代沉积中心;南水道是泥沙输运出湾的主通道,局部略微侵蚀.湾内涨、落潮流路的平面分异和地形条件的制约是北水道淤积的主要原因,强劲的落潮流以及径流是南水道成为泥沙输运主通道的主要动力条件.     

莱州湾东部外航道回淤预测及影响因素

为探讨外航道回淤特征,采用二维波浪潮流泥沙数学模型,模拟研究了莱州湾东部航道回淤情况并探讨了其影响因素,以期对航道泥沙输运研究提供借鉴。研究表明,正常天气下,水流跨越航道,流速减小、挟沙能力下降导致的悬沙落淤是航道淤积的主要原因,但淤积量有限。大风浪是造成航道淤积的主要动力因素,其淤积泥沙主要来源于海底侵蚀来沙,河流来沙和沿岸输沙对航道淤积的贡献不大。从水深地形、泥沙来源、底质类型、水文动力条件等方面分析,航道发生骤淤的可能性较小。     

粤西水东湾现代沉积环境特征与泥沙搬运路径

对粤西水东湾沉积地貌单元的现代沉积物分布特征分析与泥沙净搬运矢量计算表明，滨面斜坡沉积物主要由砂粒级物质组成，粒级参数Ｍｄ，ＱＤ和ＳＫ具有从海向岸、自东向西变化的总趋势，泥沙净搬运趋势以向岸和西北为主。落潮三角洲沉积物较其邻近滨面斜坡有所粗化，分选从中部向两侧变好，泥沙在落潮流与波浪驱动下沿落潮三角洲边缘向西运动。口门内潮汐通道深槽泥沙净搬运趋势指向湖。湖区的沉积物以泥质为主，分选中等至差，并形成绕涨潮三角洲的泥沙环流元。     

三门湾的悬沙分布和输移特性

本文根据实测资料,通过悬沙浓度ρ、流速v和水深H的对应分析,得出了三门湾的悬沙浓度分布遵循着ρ∝f(v~2/H)的规律;同时发现湾外海域有着良好的将悬沙输移入湾的动力条件,是三门湾悬沙来源的主要场所;经全潮单宽净输沙量计算表明:进出海域的悬沙净输移量不大,全湾的悬沙输移具有深槽输向边滩、南进北出的趋势,与口外海域的泥沙存在着活跃的交换。通过摩阻流速计算得到三门湾变化的总趋势是:深槽略受冲刷,滩涂缓慢淤涨,入湾通道处于动态平衡中。     

Morphodynamic Processes of Tidal Inlet and Ebb-Tidal Delta of Shuidong Bay

Based on the observed data in 1982- 1985 at Shuidong Bay area, west Guangdong Province, the morphodynamic processes of tidal inlet and ebb-tidal delta in the barrier-lagoon system are presented, including the dynamic features of tides and in the tidal inlet, the regional dyanmics and longshore sediment transport in the ebb-tidal delta, the genesis of the entrance bar, the recent erosion and deposition in the ebb-tidal delta and so on. The paper attempts to answer two questions, i. e., the stability of the tidal inlet and the feasibility of dredging on the entrance bar for the course of Shuidong Harbour. The results show that the stability of the tidal inlet is ideal and that dredging action on the entrance bar may be successful if dredging is deep enough and the course position reasonable.     

湛江港潮汐汊道落潮三角洲动力场模拟和沉积动态分析

用数值模拟方法揭示湛江港潮汐汊道落潮三角洲的潮流场特征和波浪场特征,探讨落潮三角洲地貌的形成、演化过程中的沉积动力学意义,并提出湛江港落潮三角洲沉积物的运动模式。     

Evidence for sediment recirculation on an ebb-tidal delta of the East Frisian barrier-island system, southern North Sea

The Otzum ebb-tidal delta, located between Langeoog and Spiekeroog islands along the East Frisian barrier-island coast, southern North Sea, was investigated with respect to its morphological evolution, sediment distribution patterns and internal sedimentary structures. Bathymetric charts reveal that, over the last 50 years, the size of the Otzum ebb-tidal delta has slightly shrunk, while sediment has accreted on the ebb-delta lobe to the east of the main inlet channel (west of Spiekeroog). Swash bars superimposed on the eastern ebb-tidal shoal (Robben Plate) have migrated south or south-eastwards, i.e. towards the inlet throat. The main ebb-delta body is composed of fine quartz sand, whereas the superimposed swash bars and the inlet channel bed consist of medium-grained quartz sand containing high proportions of coarser bioclastic material. Internal sedimentary structures in short box-cores (up to 30 cm long) are dominated by flood-oriented cross-beds. Longer vibro-cores (up to 1.5 m long) show that, at depth, the sediment is dominated by storm-generated parallel (upper plane bed) laminations with intercalated shell layers and dune cross-bedding. The cross-bedded sands in both box-cores and vibro-cores from the ebb-delta shoal predominantly dip towards the south or southeast, indicating transport towards the inlet throat by the flood current. The observations demonstrate that, contrary to previous contentions, the sediments of the highly mobile swash bars do not bypass the inlet but are instead being continually recirculated by the combined action of tidal currents and waves. In this model, the cycle begins with both fine and medium sands, including shell hash, being transported seawards in the main ebb channel until they reach the shallow ebb-delta front. From here, the sediment is pushed onto the eastern ebb-delta shoal by the flood current assisted by waves, becoming strongly size-sorted in the process. The medium sands together with the shell hash are formed into swash bars which migrate along arcuate paths over a base of fine sand back to the main ebb channel located south of the ebb delta. By the same token, the fine sand between the swash bars is transported south-eastwards by the flood current in the form of small dunes until it cascades into the large flood channel located to the west of Spiekeroog. From here, the fine sand is fed back into the main ebb channel, thus completing the cycle. No evidence was found on the ebb delta for alongshore sediment bypassing.     

舟山岱山水道西部海床冲淤演变分析

根据1979,1996和2009年3个时期水深地形数据,利用GIS软件分析了岱山水道西部潮滩、水下岸坡和深槽区2个时段的冲淤变化。结果显示:1979-1996年的17 a间,研究区大部分区域冲淤幅度-般在±1 m以内,只有深槽局部区域冲刷大于2 m;1996-2009年的13 a间,潮滩区冲淤变化与1979-1996年间类似,有±1 m冲淤变化,而水下岸坡和深槽区的冲刷幅度明显加大,水下岸坡平均冲刷幅度达2 m,深槽区平均冲刷幅度达3 m。据分析, 1996年以后,水下岸坡和深槽区冲刷幅度明显加大的主要原因有两个:-是岱山水道水流流速较快,粘土质的底质容易遭受冲刷;另-个是在潮滩区至水下岸坡间建设了码头和栈桥,浅水区水流部分受阻,导致深水区域流速加大,从而加剧了水下岸坡和深槽区域的冲刷幅度。     

Modelled channel patterns in a schematized tidal inlet

Tidal inlets in the Dutch Wadden Sea show typical morphological features, i.e. westward oriented main inlet channel and ebb-tidal delta. The objective of this study is to find the governing physical processes of these morphological features. The study uses a 2DH process-based morphodynamic model (Delft3D) on a schematized model domain, with dimensions similar to the Ameland inlet in the Dutch Wadden Sea.Starting from a flat bed the models are forced by tides only. Short-term simulations are made to explore the hydrodynamic characteristics and initial sedimentation and erosion patterns. Long-term morphodynamic simulations are employed to investigate the governing parameters of the main inlet channel and the ebb-tidal delta evolution. Sensitivity of the evolution is described in terms of initial inlet width (1.0 km and 3.5 km), direction and asymmetry of tidal forcing (M₂, M₄), transport formulations (Van Rijn, 1993; Engelund and Hansen, 1967) and relative position of the tidal basin with respect to the inlet (East (existing), Middle, and West).The results tend to produce morphological features typical to the Ameland inlet. The direction of tidal forcing is the main governing parameter to the present orientation of the main inlet channel and the ebb-tidal delta. The model results generally prove the conceptual hypotheses that describe the orientation of the main inlet channel and the ebb-tidal delta.     

辽河油田太—葵管道路由区海底冲淤变化研究

辽河油田太—葵管道路由区位于辽东湾顶潮汐水道区。通过不同时期实测水深对比,得出该区海底冲淤变化趋势:海区总体呈微淤态势,潮汐水道两侧浅滩淤积,两侧边坡一侧侵蚀另一侧淤积,发生平面迁移。管道路由一线蚀淤幅度较小,一般不超过0.5 m,最大侵蚀区发生在水道底和两侧边坡,是海底输油管道容易冲刷悬空的潜在危险区,需采取深埋措施提高安全性。     

港湾深槽骤淤的条件探讨

深槽骤淤指深槽底部在特定条件下产生的快速淤积,通常以浮泥形式出现.综合分析杭州湾、三门湾和象山港的地形地貌、水文泥沙及深槽固定剖面风暴前后或大、小潮期间的地形变化得出港湾深槽产生骤淤的基本条件:(1)有丰富的细颗粒物质的供应源;(2)迅速衰减的动力条件;(3)存在明显的负地形.三个条件必须同时得到满足,深槽才能产生骤淤.杭州湾泥沙来源丰富,终年悬沙浓度高,东试挖槽附近受长江冲淡水次级锋面和钱塘江冲淡水锋面影响较大,因此在一个大小潮周期内水动力条件减弱时挖槽处可产生骤淤.三门湾泥沙来源较丰富,正常天气的年份内潮滩处于缓慢淤积状态,而深槽处于冲淤基本平衡状态,但在风暴等灾害性天气下发生强烈的滩、槽泥沙交换,若风暴后处于中小潮汛期则深槽发生骤淤.象山港由于环境隐蔽,水清沙少,沿岸潮滩狭窄,缺少骤淤的物源,即使风暴作用后鹰龙山深槽也没有产生骤淤.     

曹妃甸老龙沟动力地貌体系及演化

老龙沟为典型沙坝-泻湖型潮汐汊道,潮汐汊道地貌结构完整.老龙沟口门处潮流动力最强,发育-20m的深槽.口门内涨潮流三角洲上发育完整的多级水道体系.口门外落潮三角洲止于-11 m水深处.以突起的末端坝为地形标志,落潮主水道偏于落潮三角洲东侧发育,落潮三角洲西侧发育宽缓冲流平台.落潮主水道以落潮流为优势,冲流平台上潮流动力...     

Morphodynamics of ebb-tidal deltas: a model approach

The results of 2DH numerical models of the Frisian Inlet (located in the Dutch Wadden Sea) are discussed to gain further knowledge about the physical mechanisms causing the presence of both ebb-tidal deltas and of channels and shoals in tide-dominated inlet systems. A hydrodynamic model, extended with sediment transport formulations, was used to verify earlier conceptual models that deal with ebb-tidal delta characteristics. The model does not confirm their hypothesis concerning the observed spatial asymmetry of ebb-tidal deltas and suggests that long-term morphological simulations are needed to understand this aspect. Furthermore, the model indicates that the initial formation of the ebb-tidal delta is mainly due to convergence of the tidally averaged sediment flux related to residual currents, whilst the net sediment transport in the basin is mainly caused by tidal asymmetry. A second model (accounting for feedbacks between tidal motion and the erodible bottom) was used to simulate the long-term bathymetric evolution of the Frisian Inlet under fair weather conditions. This model reproduces the gross characteristics of the observed morphology: the presence of a double-inlet system with two distinct ebb-tidal deltas having different sizes and the presence of channels and shoals. The role of the ‘Engelsmanplaat’, a consolidated shoal in the middle of the Frisian Inlet, was not found to be crucial for the morphodynamic stability of this inlet system.