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泉州湾泥沙运移特征的初步研究 总被引：4，自引：0，他引：4
泉州湾属于潮流、径流和波浪综合作用下的山地海湾，根据两次(1994年6月和2001年12月)水文泥沙实测资料，分析泉州湾悬浮泥沙和沉积物分布特征，研究其沉积物来源，并探讨北水道的沉积速率。悬浮泥沙含量自河口(湾顶)-湾口-外海逐渐降低。高值区出现在水道和河口，冬季高于夏季，大、中潮高于小潮。泉州湾沉积物分布与水动力强弱环境呈很好的对应关系。晋江携带入海的泥沙是研究区的主要物源：海岸侵蚀来沙与湾外来沙也提供了部分物源。南、北水道分别属于落潮槽与涨潮槽两种不同性质的水道。北水道沉积物较细，以沉积作用为主，其入口处淤积程度较轻，而在上游淤积程度相对较重；南水道流速较大，沉积物较粗，是泥沙输运主要通道，地形变化不明显。 相似文献
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基于2014年12月在福宁湾附近海域8个站位的同步水文泥沙观测资料,分析了冬季大潮期悬浮泥沙分布以及输运通量的变化规律,并结合理查森数、水体混合所需的势能、潮动力引起的水体势能变化率的计算结果,初步探讨了水体的垂向混合对于悬浮泥沙垂向分布的影响,研究了悬浮泥沙的输运机制。结果表明,从湾内到湾外,温度、盐度总体上呈现递增的趋势;平面上各站位悬浮泥沙浓度由湾内向湾外递减;潮周期内悬浮泥沙浓度变化存在不对称性,总体来说,湾内及湾口处(1#站除外)涨潮阶段悬浮泥沙浓度高,湾外(4#站除外)落潮阶段悬浮泥沙浓度较高。从湾内向湾外,随着水深的增加潮周期内水体的垂向混合逐渐减弱,悬沙浓度的垂向差异逐渐增大。悬浮泥沙输运在湾内及湾口整体表现为向陆输运,在湾外为向海输运。在湾内及湾口处,各分层悬浮泥沙的输运方向大多向陆,且量值较高,而湾外的悬浮泥沙输运方向在垂向上存在差异。由于潮流不对称以及悬浮泥沙的滞后效应引起的潮泵项输运对总的悬浮泥沙通量起主要贡献。 相似文献
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辽东湾绥中海岸演变及悬沙分布特征的遥感分析 总被引：6，自引：0，他引：6
本文利用辽东湾绥中地区22个年度(1975～1997年)的多时相卫星资料,分析绥中海岸自芷锚湾至狗河口约30km岸线的动态特征、近岸泥沙运动特点和悬浮泥沙的分布状况。所得结果表明,该段海岸近期处于相对稳定状态,近岸悬浮泥沙浓度较小,一般在10～50mg／L范围,是建设大中型海港码头的可选优良岸段。此外,通过遥感图象处理并结合现场调查,分析了近期近岸输沙特征和已建码头突堤堤根岸线淤涨特征,指出绥中沿岸输沙的主要方向是自西向东。 相似文献
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厦门嵩屿附近水域洪水期悬浮泥沙活动的特征 总被引：2，自引：1，他引：2
本文根据1984～1986年5次水文泥沙观测资料,研究了福建厦门嵩屿附近水域洪水期悬浮泥沙对河口三角洲和厦门西港东渡以南海域的淤积作用。 相似文献
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长江口水体表层悬浮泥沙时空分布对环境演变的响应 总被引：3，自引：2，他引：1
基于1974-2009年15个时相的陆地卫星影像,采用Gordon模型在长江口地区开展了悬浮泥沙浓度反演研究。对反演结果的时空分布规律分析表明:近40 a来长江口悬浮泥沙浓度最大下降幅度达40%;悬浮泥沙浓度演化规律与长江口来沙量变化规律具有较好的相关性;曲线拐点与2003年的长江截流、2006年三峡水库蓄水等重大工程事件吻合良好。在忽略波浪、地形等影响因素的情况下,在长时间跨度范围内,遥感技术反演的长江口悬浮泥沙浓度对长江流域环境变迁与人类水利工程活动响应敏感,较好的揭示了环境的变迁。 相似文献
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利用遥感技术估测水体中的悬浮泥沙的浓度已经成为一门成熟的技术，但将其应用于河口地区悬浮泥沙的监测仍然存在一些限制。限制之一是遥感数据（例如MODIS）的空间分辨率太低，不适合应用于河口等狭小水域的监测。相比较而言，Hyperion高光谱遥感数据有196个波段，覆盖400-2500nm的光谱范围，光谱分辨率为10nm,空间分辨率为30m，其高光谱分辨率及高空间分辨率，显示了其在河口水体悬浮泥沙遥感中的巨大潜力。利用2006年12月4号的Hyperion数据、同步实测的高光谱数据及悬浮泥沙浓度数据，对珠江口海域悬浮泥沙浓度进行了研究。利用混合光谱分解模型计算了珠江口悬浮泥沙浓度的分布。分析结果表明，混合光谱分解模型可以作为遥感监测水体悬浮泥沙浓度的定量模型。 相似文献
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底边界层水沙观测系统和应用 总被引：2，自引：0，他引：2
利用现代先进的光学和声学测量仪器(ADP、PC-ADP、ADV、OBS等),组制四角架观测系统用于底边界层的水沙观测.此观测系统既可获取垂向流速场,更可获取常规水文观测难以获取的高分辨率的近底流速、近底单点紊动过程、近底温盐沙和波浪过程.利用此观测系统于2007年8月在长江口北槽最大浑浊带内进行了实地观测.分析四角架观测数据与同步船测底部数据表明,四角架观测系统在近底(特别是底部明显分层)观测时表现出明显优势.常规水文观测测得底部含沙量一般只相当于距底70～120 cm高度含沙量;船测底部最大含沙量为5.8 kg/m 3,而架测距底30 cm处最大含沙量有25 kg/m 3;近底含沙量较高时往往出现强分层,强分层时实测距底30 cm处含沙量可达距底120 cm处含沙量的5倍;船测底部流速比架测距底30 cm处流速平均偏大45%;但距底30 cm处最大流速仍可达1.2 m/s.船测数据也验证了四角架观测数据的正确性. 相似文献
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Large Eddy Simulation for Plunge Breaker and Sediment Suspension 总被引：1，自引：1，他引：1
Breaking waves are a powerful agent for generating turbulence that plays an important role in many fluid dynamical processes, particularly in the mixing of materials. Breaking waves can dislodge sediment and throw it into suspension, which will then be carried by wave-induced steady current and tidal flow. In order to investigate sediment suspension by breaking waves, a numerical model based on large-eddy-simulation (LES) is developed. This numerical model can be used to simulate wave breaking and sediment suspension. The model consists of a free-surface model using the surface marker method combined with a two-dimensional model that solves the flow equations. The turbulence and the turbulent diffusion are described by a large-eddy-simulation (LES) method where the large turbulence features are simulated by solving the flow equations, and a subgrid model represents the small-scale turbulence that is not resolved by the flow model. A dynamic eddy viscosity subgrid scale stress model has been used for the 相似文献
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This paper presents a wave-resolving sediment transport model, which is capable of simulating sediment suspension in the field-scale surf zone. The surf zone hydrodynamics is modeled by the non-hydrostatic model NHWAVE (Ma et al., 2012). The turbulent flow and suspended sediment are simulated in a coupled manner. Three effects of suspended sediment on turbulent flow field are considered: (1) baroclinic forcing effect; (2) turbulence damping effect and (3) bottom boundary layer effect. Through the validation with the laboratory measurements of suspended sediment under nonbreaking skewed waves and surfzone breaking waves, we demonstrate that the model can reasonably predict wave-averaged sediment profiles. The model is then utilized to simulate a rip current field experiment (RCEX) and nearshore suspended sediment transport. The offshore sediment transport by rip currents is captured by the model. The effects of suspended sediment on self-suspension are also investigated. The turbulence damping and bottom boundary layer effects are significant on sediment suspension. The suspended sediment creates a stably stratified water column, damping fluid turbulence and reducing turbulent diffusivity. The suspension of sediment also produces a stably stratified bottom boundary layer. Thus, the drag coefficient and bottom shear stress are reduced, causing less sediment pickup from the bottom. The cross-shore suspended sediment flux is analyzed as well. The mean Eulerian suspended sediment flux is shoreward outside the surf zone, while it is seaward in the surf zone. 相似文献
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Based on a wave bottom boundary layer model and a sediment advection-diffusion model, seven turbulence schemes are compared regarding their performances in prediction of near-bed sediment suspension beneath waves above a plane bed. These turbulence algorithms include six empirical eddy viscosity schemes and one standard two-equation k-ε model. In particular, different combinations of typical empirical formulas for the eddy viscosity profile and for the wave friction factor are examined. Numerical results are compared with four laboratory data sets, consisting of one wave boundary layer hydrodynamics experiment and three sediment suspension experiments under linear waves and the Stokes second-order waves. It is shown that predictions of near-bed sediment suspension are very sensitive to the choices of the empirical formulas in turbulence schemes. Simple empirical turbulence schemes are possible to perform equally well as the two-equation k-ε model. Among the empirical schemes, the turbulence scheme, combining the exponential formula for eddy viscosity and Swart formula for wave friction factor, is the most accurate. It maintains the simplicity and yields identically good predictions as the k-ε model does in terms of the wave-averaged sediment concentration. 相似文献
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《Coastal Engineering》2001,42(2):173-197
Intra-wave sediment suspension is examined using high-resolution field measurements and numerical hydrodynamic and sediment models within 120 mm of a plane seabed under natural asymmetric waves. The detailed measurements of suspended sediment concentration (at 5 mm vertical resolution and at 4 Hz) showed two or three entrainment bursts around peak flow under the wave crest and another at flow reversal during the decelerating phase. At flow reversal, the mixing length was found to be approximately double the value attained at peak flow under the crest. To examine the cause of multiple suspension peaks and increased diffusion at flow reversal, a numerical “side-view” hydrodynamic model was developed to reproduce near-bed wave-induced orbital currents. Predicted currents at the bed and above the wave boundary layer were oppositely directed around flow reversal and this effect became more pronounced with increasing wave asymmetry. When the predicted orbital currents and an enhanced eddy diffusivity during periods of oppositely directed flows were applied in a Lagrangian numerical sediment transport model, unprecedented and extremely close predictions of the measured instantaneous concentrations were obtained. The numerical models were simplified to incorporate only the essential parameters and, by simulating at short time scales, empirical time-averaged parameterisations were not required. Key factors in the sediment model were fall velocities of the full grain size distribution, diffusion, separation of entrainment from settlement, and non-constant, but vertically uniform, eddy diffusivity. Over the plane bed, sediment convection by wave orbital vertical currents was found to have no significant influence on the results. 相似文献
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Wiebe P.H. Stanton T.K. Benfield M.C. Mountain D.G. Greene C.H. 《Oceanic Engineering, IEEE Journal of》1997,22(3):445-464
High-frequency (120 and 420 kHz) sound was used to survey sound scatterers in the water over Georges Bank. In addition to the biological sound scatterers (the plankton and micronekton), scattering associated with internal waves and suspended sediment was observed. Volume backscattering was more homogeneous in the vertical dimension (with occasional patches) in the shallow central portion of the Bank where there is significant mixing. In the deeper outer portion of the Bank where the water is stratified, volume backscattering was layered and internal waves modulated the vertical position of the layers in the pycnocline. The internal waves typically had amplitudes of 5-20 m, but sometimes much higher. Species composition and size data from samples of the animals and suspended sediment used in conjunction with acoustic scattering models revealed that throughout the region the animals generally dominate the scattering, but there are times and places where sand particles (suspended as high as up to the sea surface) can dominate. The source of the scattering in the internal waves is probably due to a combination of both animals and sound-speed microstructure. Determination of their relative contributions requires further study 相似文献
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Owing to lack of observational data and accurate definition,it is difficult to distinguish the Kuroshio intrusion water from the Pacific Ocean into the South China Sea(SCS).By using a passive tracer to identify the Kuroshio water based on an observation-validated three-dimensional numerical model MITgcm,the spatio-temporal variation of the Kuroshio intrusion water into the SCS has been investigated.Our result shows the Kuroshio intrusion is of distinct seasonal variation in both horizontal and vertical directions.In winter,the intruding Kuroshio water reaches the farthest,almost occupying the area from 18°N to 23°N and 114°E to 121°E,with a small branch flowing towards the Taiwan Strait.The intrusion region of the Kuroshio water decreases with depth gradually.However,in summer,the Kuroshio water is confined to the east of 118°E without any branch reaching the Taiwan Strait;meanwhile the intrusion region of the Kuroshio water increases from the surface to the depth about 205 m,then it decreases with depth.The estimated annual mean of Kuroshio Intrusion Transport(KIT) via the Luzon Strait is westward to the SCS in an amount of –3.86×106 m3/s,which is larger than the annual mean of Luzon Strait Transport(LST) of –3.15×106 m3/s.The KIT above 250 m accounts for 60%–80% of the LST throughout the entire water column.By analyzing interannual variation of the Kuroshio intrusion from the year 2003 to 2012,we find that the Kuroshio branch flowing into the Taiwan Strait is the weaker in winter of La Ni?a years than those in El Ni?o and normal years,which may be attributed to the wind stress curl off the southeast China then.Furthermore,the KIT correlates the Ni?o 3.4 index from 2003 to 2012 with a correlation coefficient of 0.41,which is lower than that of the LST with the Ni?o 3.4 index,i.e.,0.78. 相似文献
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山东半岛东北部海域悬浮体季节分布及控制因素 总被引：1，自引：0，他引：1
基于2018年山东半岛东北部海域冬、夏两季悬浮体浓度、浊度及水温和盐度调查资料,分析了研究区水体悬浮体浓度的季节性变化,探讨了其控制因素。结果表明:夏季浊度在0.2~37.8FTU之间变化,冬季浊度在1.5~100.1FTU之间变化,均表现为底高表低、东高西低的特征。夏季水温分层明显,表现为表层高、底层低的特征,盐度整体无明显变化;冬季温盐垂向上混合均匀,平面上表现为近岸低温低盐水体向远岸高温高盐水体的过渡。悬浮体浓度分布受潮流、波浪、温跃层和温盐锋面等因素影响。夏季,悬浮体垂向上受到温跃层影响,底层悬浮体难以向表层输运;平面上潮混合和波浪差异性作用阻碍了悬浮体的水平输运。冬季,强风浪促使悬浮体垂向混合剧烈,表层悬浮体浓度明显较夏季变高;平面上沿岸流和黄海暖流形成的温、盐锋面阻碍了水团间悬浮体的输运。 相似文献
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Sheet flow and suspension of sand in oscillatory boundary layers 总被引：1，自引：0，他引：1
after revisionTime-dependent measurements of flow velocities and sediment concentrations were conducted in a large oscillating water tunnel. The measurements were aimed at the flow and sediment dynamics in and above an oscillatory boundary layer in plane bed and sheet-flow conditions. Two asymmetric waves and one sinusoidal wave were imposed using quartz sand with D50 = 0.21 mm. A new electro-resistance probe with a large resolving power was developed for the measurement of the large sediment concentrations in the sheet-flow layer. The measurements revealed a three layer transport system consisting of a pick-up/deposition layer, an upper sheet flow layer and a suspension layer.In the asymmetric wave cases the total net transport was directed “onshore” and was mainly concentrated in the thin sheet flow layer (< 0.5 cm) at the bed. A small net sediment flux was directed “offhore” in the upper suspension layer. The measured flow velocities, sediment concentrations and sedimenl fluxes showed a good qualitative agreement with the results of a (numerical) 1DV boundary-layer flow and transport model. Although the model did not describe all the observed processes in the sheet-flow and suspension layer, the computational results showed a reasonable agreement with measured net transport rates in a wide range of asymmetric wave conditions. 相似文献