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1.
基于实测的水深、潮流、悬浮体、底质数据及历史气象资料等,采用导入SWAN波浪参数的ECOMSED三维模型,模拟大风浪对小清河口附近海域悬浮体浓度和底床冲淤变化的影响程度。并利用全潮水文观测资料对水动力和输沙率模拟结果进行检验,对比分析表明计算值与实测值吻合良好。模拟结果表明,大风浪影响下近岸海域泥沙输运变化较大,悬浮体浓度可达一般天气的10倍左右,而底床冲淤变化可达平时的百余倍。大风浪期间剧烈的底床冲淤变化对河口拦门沙演化影响较大。 相似文献
2.
渤海湾曹妃甸老龙沟海区属于典型的离岸沙坝-泻湖海岸体系,口门处发育有拦门沙。采用实测资料分析和二维波流泥沙数学模型计算研究了拦门沙成因及其开挖后的回淤情况。研究表明,涨落潮流路不一致、落潮流扩散是老龙沟拦门沙形成的主要原因。针对该海区波浪、潮流、泥沙及海床演变特点,进行了2006年、2007年大小潮潮流泥沙的验证及2008年8~12月试挖槽回淤的验证,在此基础上,预测了拦门沙航道正常情况下的泥沙回淤和大风天骤淤。试挖槽监测资料分析及数学模型计算表明,风浪掀沙是影响老龙沟拦门沙回淤的重要因素。 相似文献
3.
渤海湾曹妃甸老龙沟海区属于典型的离岸沙坝-潟湖海岸体系,口门处发育有拦门沙。采用实测资料分析和二维波流泥沙数学模型计算研究了拦门沙成因及其开挖后的回淤情况。研究表明,涨落潮流路不一致、落潮流扩散是老龙沟拦门沙形成的主要原因。针对该海区波浪、潮流、泥沙及海床演变特点,进行了2006年、2007年大小潮潮流泥沙的验证及2008年8~12月试挖槽回淤的验证,在此基础上,预测了拦门沙航道正常情况下的泥沙回淤和大风天骤淤。试挖槽监测资料分析及数学模型计算表明,风浪掀沙是影响老龙沟拦门沙回淤的重要因素。 相似文献
4.
岛屿海岸所处的水动力泥沙环境以及工程实施后引起的相关变化都具有自身的独特性和复杂性。根据历史资料,在对嵊泗中心渔港海区已建工程影响下的水沙动力过程变化深入分析的基础上,利用波浪和潮流共同作用下的二维泥沙数学模型,对拟建工程引起的潮流场、含沙量场以及海床冲淤变化进行了分析和预测。研究表明,已建与拟建防波堤工程会引起港区水动力减弱,海床演变以淤积作用为主,年淤积强度0.1~0.3 m;已围与拟围海造地工程则会束窄潮流通道,导致水动力增强,海床以轻微冲刷为主。拟建工程与已建工程作用下的水沙动力过程具有良好的类比性。 相似文献
5.
极端天气条件下,波浪引起的高含沙水体会引起航道骤淤,增大航道回淤量。以"马勒卡"台风期间现场水文资料为基础,建立了波流共同作用下的长江口三维潮流泥沙数学模型,研究北槽航道骤淤问题。数学模型验证了"马勒卡"台风期间的北槽水沙过程,相似性较好,通过分离波浪,探讨了潮流与波流共同作用下的含沙量及航道淤积分布差异,研究了台风浪对航道骤淤的影响。研究表明,台风浪对-15 m等深线以浅水域含沙量影响较大,北槽含沙量自上游至口外逐渐增大,改变了常态天气北槽"中间高、两头低"的含沙量分布趋势。台风浪对北槽口内航道回淤分布影响较小,北槽口外航道淤积量剧增,即航道骤淤主要发生在北槽口外。 相似文献
6.
曹妃甸老龙沟潮汐通道拦门沙演变机制 总被引：2，自引：0，他引：2
渤海湾曹妃甸老龙沟海区属于泻湖型潮汐通道体系,口门附近发育有大规模拦门沙浅滩。由于沿岸泥沙供给不足,近几十年来东坑坨等沙坝外侧海区整体呈侵蚀冲刷态势,等深线向陆蚀退。老龙沟西支深槽也以侵蚀作用为主,而拦门沙地区滩槽冲淤变化则与东坑坨演变密切相关。其中东槽冲刷发展主要是东坑坨西南尾端淤长压迫老龙沟口门,引起岬角效应增大、潮流动力增强所致,而西槽的摆动现象则主要与东槽发展所产生的挤压作用有关。由于泥沙供给不足,近年来东槽发展和西槽摆动的速度都有明显减缓。 相似文献
7.
大量波流相互作用的实验表明,当波浪顺流传播时,平均水面附近的流速减小,而当波浪逆流传播时,平均水面附近的流速增加.为了从理论上解释这种现象,从垂向二维Navier-Stokes方程出发,推导出波浪、潮流共同作用下的水流控制方程;采用微幅波理论简化控制方程,并引入Grant-Madsen波流边界层模型,得到波流共同作用下的紊动切应力及流速垂线分布表达式.通过和实验结果及数值结果的对比,结果预测值和实测值较为吻合,表明公式能反映波高变化及涡粘系数共同对流速垂线分布的影响,且简单实用.利用该公式分析了波浪顺流、逆流流速变化的原因. 相似文献
8.
从波浪引起的海床内部渗流与床面泥沙运动耦合的角度出发,研究波浪作用下海床临界冲刷机理及计算方法。研究表明,波浪作用下床面泥沙起动及冲刷是一个不断向下发展的过程,最终达到一个临界冲刷深度。波浪引起的渗流力能够显著降低泥沙的临界起动切应力,促进泥沙起动,是影响海床冲刷的一个重要因素。将渗流力引入到传统泥沙起动公式中,推导并给出了波浪作用下海床临界冲刷深度的计算方法。结合室内和现场两个算例,很好地解释了波浪水槽试验中海床"流化"现象和黄河水下三角洲粉砂流冲沟等灾害地貌特征及成因,初步验证了该方法用于评价和计算海床冲刷的有效性。 相似文献
9.
考虑渗流力的海床临界冲刷机理及计算方法 总被引：1，自引：0，他引：1
从波浪引起的海床内部渗流与床面泥沙运动耦合的角度出发,研究波浪作用下海床临界冲刷机理及计算方法。研究表明,波浪作用下床面泥沙起动及冲刷是一个不断向下发展的过程,最终达到一个临界冲刷深度。波浪引起的渗流力能够显著降低泥沙的临界起动切应力,促进泥沙起动,是影响海床冲刷的一个重要因素。将渗流力引入到传统泥沙起动公式中,推导并给出了波浪作用下海床临界冲刷深度的计算方法。结合室内和现场两个算例,很好地解释了波浪水槽试验中海床"流化"现象和黄河水下三角洲粉砂流冲沟等灾害地貌特征及成因,初步验证了该方法用于评价和计算海床冲刷的有效性。 相似文献
10.
为适应伶仃洋茅洲河口治理开发条件,以保证行洪顺畅为泄洪纳潮的首要原则,同时顺应水沙运动和河势发展规律,对河口进行治导线比选和优化。该河口治导线方案分单、双通道,两类通道不同扩宽率下设计有围填、围填加开挖2种方案,开展水动力泥沙数学模拟计算和物理模型试验。结果表明:河口治导线各方案对伶仃洋涨、落潮流速的影响范围主要集中在交椅湾及其附近海域;方案实施后,周边海区冲淤变化较小,未对河势造成不利影响;根据对水动力、河口泄洪、河势稳定影响的综合分析,单双通道相比较而言,对洪水位、纳潮量、高低潮位、流速、河床冲淤的影响规律具有较好的一致性,相同扩宽率下各方案的影响程度均在同量级。 相似文献
11.
为了评估港珠澳大桥人工岛建设对周边海区水沙动力环境的影响,针对人工岛设计及工程海区水沙特性,建立了整体潮流泥沙物理模型,系统研究了人工岛建设引起的动力地貌演变效应。试验结果表明,受岛体阻水影响,潮流在人工岛两端分别形成双向绕流,流速明显增大,并在岛桥结合部与岛隧结合部发育局部冲刷坑;人工岛背水面同时存在多个大小不一的强紊动小尺度回流,并具有不断形成、发育、发展到消亡的周期性变化过程。受人工岛自身位置、形态、尺度以及工程海区地形、水流、泥沙等因素影响,港珠澳大桥东、西两个人工岛引起的动力地貌演变效应,既在变化规律上具有较好的一致性,又在影响形式与程度上存在明显的差异性。 相似文献
12.
曹妃甸浅滩潮道保护意义及曹妃甸新老填海规划对比分析 总被引：1，自引：0，他引：1
曹妃甸填海工程是全国第一大填海工程,拟填海造陆310 km2,建设曹妃甸工业区。曹妃甸海区有曹妃甸外缘深槽和老龙沟深槽两大港口潜力区,建设曹妃甸工业区,使其充分发挥优良港口的作用是合理的。但填海面积过大,填挖土石方严重不平衡,尤其是通岛公路的建设阻断了曹妃甸浅滩潮道是曹妃甸老填海规划的主要缺陷。曹妃甸浅滩潮道是浅滩区的重要潮流通道,对维护老龙沟深槽港口潜力区和区域海洋环境有重要作用,不应被阻断而应当保留畅通。海洋专家们的呼吁对曹妃甸填海规划的修改起了重要作用。近来出台的曹妃甸新填海规划做了重大修改:准备再开通浅滩潮道,恢复北东东向的浅滩潮流系统;要在老龙沟附近修建一个大港池,使老龙沟深槽港口潜力区得到保护和利用;填挖土石方平衡有了明显改善;增加了岸线;减轻了对海洋环境的影响。但仍然存在某些需要进一步完善和推敲之处。津塘—曹妃甸地区是中国两大地面沉降区之一,应做好防止地面沉降、海洋灾害及地震灾害等隐患的准备。填海面积不宜过大,少填多察,多做海洋环境检测。填海要在海洋环境容量能够承受的情况下循序渐进地进行。 相似文献
13.
河口入海泥沙沉积固结过程中抗侵蚀性的变化直接决定着沉积物的再悬浮和二次迁移,对河口岸滩的稳定具有重要决定作用。在现代黄河三角洲潮滩模拟入海泥沙快速沉积,现场测试不同固结时间沉积物的抗侵蚀性和物理力学指标的变化。研究发现,黄河入海泥沙沉积物的抗侵蚀性随固结时间增长迅速提高,当沉积固结时间达8h时,其临界侵蚀切应力就超过了原状潮滩表层沉积物;新沉积泥沙的临界侵蚀切应力与其重度、贯入阻力、剪切强度呈良好的正相关关系,与含水率呈良好的负相关关系。黄河入海泥沙临界侵蚀流速的试验值随固结时间的增长速率要高于各泥沙起动公式计算值的增长速率,前者是后者的1.5～4.1倍。 相似文献
14.
The relative roles of waves and tidal currents in transporting bottom sediment on the continental shelf off Lands End, southwest England, are evaluated by study of (a) sediment grain size in relation to boundary layer measurements in tidal currents, (b) regional variation in sediment parameters in relation to peak tidal and wave-induced currents, and (c) visual observation of bedforms. (a) The sediments are mainly zoogenic sands. The average hydraulic equivalent median diameter is Mdφ=1.40φ (medium grade sand), and two-thirds of the median grain sizes fall between 0.97φ and 1.83φ. The linear bottom current which will just move this range of sizes is exceeded only slightly by the highest tidal drag velocities ū* measured in the area. Thus, sediment movement by tidal currents alone is restricted to areas of high bed roughness and strong peak tidal flows. In contrast, wave-induced oscillatory currents at 100 m depth (typical of the area) attain sufficient speed to disturb the same particle sizes over 3% of the time. This includes storm periods when much greater velocities occur. (b) The average Mdφ of the sediment decreases southwest and northeast from south of the Lizard. This correlates well with the pattern of maximum tidal current speeds, suggesting that tidal currents control the areal distribution of sediment median grain size. Most sediments are well sorted (mean σi=0.48φ). Sorting improves at shallower depths but does not improve in areas of faster tidal currents, suggesting that wave-induced currents exert the major control on sorting. Silt and clay proportions increase west of the Scilly Isles and are influenced by both wave and tidal currents. (c) Photographs and television pictures show that symmetrical bedforms due to wave action are dominant north and west of the western Channel. Asymmetric bedforms are more common in the western Channel itself, where tidal currents and bed roughness are both high. Results are used to construct a sediment transport model for the study area. Since medium grade well sorted sands occur in depths of over 100 m, many ancient, extensive, well sorted sand sheets may have been deposited at depths greater than previously suspected. 相似文献
15.
通过近年来对江苏沿海有影响的台风暴潮作用前后的滩面高程观测,结合台风浪资料分析,探究了江苏中部沿海潮滩对风暴潮的响应过程。结果显示:潮滩剖面在风暴潮期间呈现"低滩侵蚀、沿岸输运、高滩稳定",明显区别于沙质海岸在台风浪作用下"高滩侵蚀、离岸输运、低滩淤积"的演变特征。应用Delft3D平面二维水沙动力数学模型,模拟了正常天气和台风浪情况下的滩面演变,从动力学角度解释了潮滩间不同区域演变特征差异的原因,论证了台风浪对地貌演变的短历时"插曲式"作用,阐明了涨潮优势流是风暴侵蚀后泥沙沿岸向输运的主控因子。 相似文献
16.
Sylvain Capo Isabelle Brenon Aldo Sottolichio Patrice Castaing Patrick Le Goulven 《Journal of African Earth Sciences》2009,55(1-2):52
In comparison to their temperate counterparts, sediment processes in tropical estuaries are poorly known and especially in African ones. The hydrodynamics of such environments is controlled by a combination of multiple processes including morphology, salinity, mangrove vegetation, tidal processes, river discharge, settling and erosion of mud and by physico-chemical processes as well as sediment dynamics.The aim of this study is to understand the sediment processes in this transitional stage of the estuary when the balance between river discharges and marine processes is reversing. Studying the hydrodynamics and sediment dynamics of the Konkouré Estuary has recently been made possible thanks to new data on bathymetry, sedimentary cover, salinity, water elevations, and current velocities. The Lower Konkouré is a shallow, funnel shaped, mesotidal mangrove-fringed, tide-dominated estuary, well mixed during low river discharge and stratified during high river discharge. The Konkouré Estuary is turbid despite the small amount of terrestrial input and its residual velocity at the mouth during low river discharges, landwards for two of the three branches, suggests a landward migration by tidal pumping of the suspended particulate matter. A Turbidity Maximum Zone (TMZ) is identified for typical states of the estuary with regard to fluvial and tidal components. Suspended sediment transport during a transitional stage between the rainy and dry seasons is known thanks to current velocity and Suspended Sediment Concentration (SSC) measurements taken in November 2003. The Richardson layered number calculation assesses that turbulence is the major mixing process in the water column, at least during the flood and ebb stages, whereas stratification occurs during the slack water periods. Tidal currents generate bottom erosion, and turbulence mixes the suspended sediment throughout the water column. As a result, a net sediment input is calculated from the western Konkouré outlet for two consecutive tidal cycles. Despite the net water export, almost 300 tons per tide reach the estuary through this outlet, for a moderate river flow. 相似文献
17.
A study of the dynamics of a marine sandwave 总被引：3，自引：0，他引：3
D. N. LANGHORNE 《Sedimentology》1982,29(4):571-594
The movement of the crest of a sandwave was studied using cross-sectional profiles obtained from lines of sea-bed reference stakes. Measurements were made, over a six month period, before and after flood and ebb tides in relation to both spring and neap tides and surface wave conditions. Additional observations were obtained on a daily basis, over an equinoctial neap to spring to neap tidal period, in conjunction with boundary layer flow measurements. Tracer experiments were conducted to study the dispersion of sediment from the sandwave crest. The results showed that the sandwave was relatively stable at neap tides, whilst at higher tidal ranges, the crest position oscillated with successive flood and ebb tides. Net flank erosion occurred on the less steep, upstream slope during the dominant ebb tide. This, together with increased deposition on the lee slope, caused the crest to advance. It was not possible to extrapolate sandwave migration over long periods as the tidal dynamic trends were interrupted by wind stress and surface wave activity. High particle orbital velocities, generated at the sea-bed by storm waves, caused major reductions in crestal heights. Calculated volumes of sediment eroded and accreted were used, with boundary layer flow measurements, to calculate threshold velocities for the movement of the sediment and sediment transport rates. 相似文献
18.
A three-dimensional, intratidal sediment transport model is developed for the estuarine turbidity maximum (ETM) in the upper
Chesapeake Bay. The model considers three particle size classes, including the fine class mostly in suspension in the water
column, the medium class alternately suspended and deposited by tidal currents, and the coarse size suspended only during
the times of relatively high energy events. Based on the results of a box model, depth-limited erosion with continuous deposition
is employed for the medium and coarse classes by varying the critical shear stress for erosion as a function of eroded mass.
For the fine class, mutually exclusive erosion and deposition is employed with a small constant value for the critical shear
stresses for erosion and deposition to assure quick erosion of recently deposited fine particles but without allowing further
erosion of consolidated bed sediments. The model is run to simulate the annual condition in 1996, and the model generally
gives a reasonable reproduction of the observed characteristics of the ETM relative to the salt limit and tidal phase. The
model results for 1996 are analyzed to study the characteristics of the ETM along the main channel of the upper bay in intertidal
and intratidal time scales. Under a low flow condition, local erosion/deposition and bottom horizontal flux convergence are
the main processes responsible for the formation of the ETM, with the settling flux confining the ETM to the bottom water.
Under a high flow condition, a distinctive ETM is formed by strong convergence of the downstream flux of sediments eroded
from the upstream of the null zone and the upstream flux of sediments settled at the downstream of the null zone. Intratidal
variation of the ETM is mainly controlled by erosion and the tidal transport of eroded sediments for a low flow condition.
Under the direct influence of a high flow event, the ETM is mainly formed by erosion during ebbing tidal current strengthened
by large freshwater discharge and by convergence of ebbing freshwater discharge and flooding tidal current. During the rebounding
stage of a high flow event, intratidal variations are mainly controlled by tidal asymmetry caused by the interaction between
tidal currents, gravitational circulation, and stratification. 相似文献