共查询到17条相似文献，搜索用时 171 毫秒
1.
利用涌浪影响下短时段内的冲流带滩面高频高程数据和碎波带波流资料,在奇异谱分析(SSA)的基础上,对比研究了不同形态滩面的冲淤变化趋势、趋势分布形状、冲淤变化周期和冲淤变化强度,以及同一条剖面不同桩点间各因素间的变化关系;用交叉谱方法探索了每分钟滩面高频冲淤变化与碎波带长重力波间的作用关系。分析结果表明,滩角韵律地形引起的冲流分流作用促进了滩脊向滩谷的泥沙转运,冲流带滩面存在明显的长重力波频段的周期性冲淤振动,滩面冲淤振动强度由滩面下部向上部递减,碎波带长重力波对滩面高频冲淤变化起重要作用。 相似文献
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海滩冲流带高频振动地形动力过程分析 总被引：1，自引：0，他引：1
在粤东汕尾后江湾海滩冲流带布设2条观测剖面,共计6个观测点,对滩面冲流带在约一个潮周期内的高频振动进行了观测,取得采样频率分别为1min/次和6min/次的滩面数据各1组.结合同步观测的碎波带波浪潮汐数据,分析探讨了海滩高频振动特征.分析认为在涌浪条件下,滩面高频振动的日内变化主要受到潮位变化过程的控制,涨潮堆积,落潮侵蚀.利用交叉谱分析的结果表明滩面高程变化滞后于潮位变化.滩面下部比上部振动幅度大,变化复杂,滩角脊部比凹部活跃.波群对滩面高频振动有显著影响,特别是波高大于有效波高的波群.滩面高频振动没有表现出明显的泥沙逐渐向陆地堆积过程,有一定的振动周期. 相似文献
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粤东后江湾涨落潮下的碎波带波能与滩面地形时空变化分析 总被引：6，自引：1，他引：5
利用涌浪和处于陡滩面、滩面下陡坎和深槽海滩地形条件下的海滩碎波带压力波和滩面地形资料,对碎波带中的入射总波能、长重力波能及两者比值随潮位涨落的变化关系,碎波带动力因子与滩面地形之间的作用关系及典型相关和多维偏交叉谱关系等作了初步分析。结果表明,碎波带中的入射总波能与潮位涨落呈现出一致的变化规律;而碎波带中的长重力波能变化与潮位涨落变化趋势相反;碎波带各动力因子、滩面潜水位和碎波带波浪、潮位及滩面地形引起的滩面陡坎处破波点位置变动等因素的耦合作用,对滩面向海发育和滩面地形变化有重要影响。 相似文献
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长重力波运动与近岸过程研究综述 总被引：4，自引：1，他引：3
简要介绍了长重力波的概念和作用,概述了近岸长重力波的运动形式、类型、分布和波能变化,分析了近岸长重力波与泥沙运动、海岸侵蚀、近岸环流系统、海滩碎波带地貌形态和潮汐等的关系,提出了进一步研究的几点建议。 相似文献
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对不同波况条件下实测的一岬间海滩碎波带两个测站的波面数据 ,通过小波变换方法计算了小波能谱 ,并作了显著性检验。结果表明 :( 1 )碎波带波能存在典型的多尺度振荡特性 ;( 2 )在正常波况下 ,波能主要分布于风浪频域 ,入射波自外测站向内测站传播过程中 ,能量具有向低频方向转移的趋势 ;( 3)在高能波况下 ,能量均向长重力波频带增加 ,在长重力波显著尺度 ,二测站之间存在良好的位相一致关系 相似文献
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一般认为滩角是近岸带泥沙、水动力和地形耦合作用的产物,对近岸带特别是碎波带和冲流带的动力变化响应迅速,还可以反映海滩状态,但具体的成因一直得不到很好的解释.首先详细介绍了关于滩角成因的争论以及自组织机制理论,其中驻立边缘波假说和自组织机制假说是最为认同的两种滩角成因假说.基于WERNER(1993)提出的滩角形成的自组织机制假说,建立包含冲流动力、泥沙输运和地形演变的滩角形成和发育的元胞自动机模型.模型中修正了以前研究中的坡度参数表达式和水动力输入方式.经过200个冲流循环的数值模拟,原来平直的滩面上形成了明显的滩角形态,滩角间距约为5.5～6.0 m,520个循环周期后,滩角形态基本上达到稳定状态.对模拟过程进行分析,结果表明:(1)模拟得到的滩角形态比先前的研究结果更接近天然状态下的滩角;(2)随机的水质点冲流运动使海滩地形呈无规律变化,但通过动力、泥沙、地形之间的反馈过程逐渐形成了滩角地形;(3)滩角形成过程中,海滩基本上处于堆积过程中.开始堆积速度较快,当滩角形态达到准平衡状态时(大约300个循环后),海滩体积增速变慢,并逐渐地达到稳定状态,海滩体积变化呈现小的波动调整;(4)模拟得到的有效冲流距离(S)和滩角间距(λ),满足滩角自组织机制假说的基本关系.因此,可以认为滩角是在海滩泥沙、地形与波、流的自组织过程中形成的,是一种堆积地形.自组织理论为从不同的侧面认识和研究海岸带现象与过程提供一扇窗口,是一个值得研究的方向. 相似文献
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粤东后江湾近岸长重力波特征分析 总被引：2，自引：0，他引：2
利用粤东后江湾近岸有限水深(包括碎波带)4个测点的压力波数据,依据波谱分析方法对4个测点的入射波有效波高、长重力有效波高、有效波陡、波面谱、谱宽度和谱尖度参量进行了统计和对比分析.分析认为,在近岸有限水深条件下,波浪由近岸(相对水深0.201)到破、碎波带运动过程中,(1)长重力波有效波高呈增大趋势,至破、碎波带位置增幅最为明显;(2)入射波有效波高至破、碎波带区域达到最大,在破波带外有限水深区域呈现先增大后减小的变化趋势;(3)有效波陡、谱宽度参数呈增大趋势;(4)波浪内部能量向高、低频段发生转移,至破、碎波带区域转移程度最为明显,在峰值频率的高、低频段形成谱峰;长重力波谱强度在破、碎波带区域明显高于对应有限水深测点. 相似文献
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广东水东湾弧形海岸切线段海滩剖面的过程分析 总被引：8，自引：1，他引：8
本文运用因子分析和交叉谱分析方法对广东水东湾晏镜海滩剖面实测数据进行了地貌过程分析.因子分析结果提取了4个主因子,累积方差达90%.这4个主因子分别代表了碎波带的脊-沟过程、冲流带的滩肩过程、引起后滨面切割的侵蚀性裂流-滩角过程和造成上部滩面净侵蚀的潮汐过程.先前波况对海滩剖面的影响通过交叉谱分析表明,平均海面以上海滩单宽体积变化落后于波能变化1.6-3.4d.海滩剖面动态分析显示平均海面以下是净侵蚀场所,平均海面以上则处于动态平衡.海滩主状态目前为脊-沟或低潮台地的中间类型. 相似文献
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《Coastal Engineering》2005,52(6):497-511
A weakly non-linear Boussinesq model with a slot-type shoreline boundary is used to simulate swash oscillations on beaches. Numerical simulations of swash were compared with laboratory measurements and in general good agreement found (less than 15% root-mean-square error of surface elevation except in regular waves). A series of numerical experiments on shoreline movement were then performed for a range of beach slopes and incident wave conditions. The resulting swash characteristics are then discussed in terms of their physical nature and spectral properties. On steep slopes, both individual bores and infragravity waves are equally significant in driving the swash while infragravity waves alone drive them on mild slopes. Swash excursions on any given slope are found to be highest when individual bores from a partially saturated surf zone ride on top of low-frequency waves. This is confirmed by the relationship found between swash excursion and wave groupiness in the surf zone. Swash excursions increase with increasing incident wave energy, even in fully saturated surf zones. However, a poor correlation is found between swash excursion and the surf similarity parameter due to the involvement of infragravity wave energy in the swash. 相似文献
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《Marine Geology》2005,216(3):169-189
Simultaneous high frequency field measurements of water depth, flow velocity and suspended sediment concentration were made at three fixed locations across the high tide swash and inner surf zones of a dissipative beach. The dominant period of the swash motion was 30–50 s and the results are representative of infragravity swash motion. Suspended sediment concentrations, loads and transport rates in the swash zone were almost one order of magnitude greater than in the inner surf zone. The vertical velocity gradient near the bed and the resulting bed shear stress at the start of the uprush was significantly larger than that at the end of the backwash, despite similar flow velocities. This suggests that the bed friction during the uprush was approximately twice that during the backwash.The suspended sediment profile in the swash zone can be described reasonably well by an exponential shape with a mixing length scale of 0.02–0.03 m. The suspended sediment transport flux measured in the swash zone was related to the bed shear stress through the Shields parameter. If the bed shear stress is derived from the vertical velocity gradient, the proportionality coefficient between shear stress and sediment transport rate is similar for the uprush and the backwash. If the bed shear stress is estimated using the free-stream flow velocity and a constant friction factor, the proportionality factor for the uprush is approximately twice that of the backwash. It is suggested that the uprush is a more efficient transporter of sediment than the backwash, because the larger friction factor during the uprush causes larger bed shear stresses for a given free-stream velocity. This increased transport competency of the uprush is necessary for maintaining the beach, otherwise the comparable strength and greater duration of the backwash would progressively remove sediment from the beach. 相似文献
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Sediment-level oscillations with heights of about 6 cm and shore-normal lengths of order 10 m have been measured in the swash zone of a high-energy, coarse-sand beach. Crests of oscillations were shore parallel and continuous alongshore. The oscillations were of such low steepness (height-to-length ratio approximately 0.006) that they were difficult to detect visually. The period of oscillation ranged between 6 and 15 min and decreased landward across the swash zone. The sediment-level oscillations were progressive landward with an average migration rate in the middle to upper swash zone of 0.8 m min−1. Migration was caused mostly by erosion on the seaward flank of the crest of an oscillation during a period of net seaward sediment transport. Thus, the observed migration was a form migration landward rather than a migration involving net landward sediment transport. The observed sediment-level oscillations were different than sand waves or other swash-zone bedforms previously described. 相似文献
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This paper builds on the work of Masselink [Masselink, G., 1993. Simulating the effects of tides on beach morphodynamics. J. Coast. Res. SI 15, 180–197.] on the use of the residence times of shoaling waves, breaking waves and swash/backwash motions across a cross-shore profile to qualitatively understand temporal beach behaviour. We use a data set of in-situ measurements of wave parameters (height and period) and water depth, and time-exposure video images overlooking our single-barred intertidal measurement array at Egmond aan Zee (Netherlands) to derive boundaries between the shoaling zone, the surf zone and the swash zone. We find that the boundaries are functional dependencies of the local relative wave height on the local wave steepness. This contrasts with the use of constant relative wave heights or water levels in earlier work. We use the obtained boundaries and a standard cross-shore wave transformation model coupled to an inner surf zone bore model to show that large (> 5) relative tide ranges (RTR, defined as the ratio tide range–wave height) indicate shoaling wave processes across almost the entire intertidal profile, with surf processes dominating on the beach face. When the RTR is between 2 and 5, surf processes dominate over the intertidal bar and the lower part of the beach face, while swash has the largest residence times on the upper beach face. Such conditions, associated with surf zone bores propagating across the bar around low tide, were observed to cause the intertidal bar to migrate onshore slowly and the upper beach face to steepen. For RTR values less than about 2, surf zone processes dominate across the intertidal bar, while the dominance of swash processes now extends across most of the beach face. The surf zone processes were now observed to lead to offshore bar migration, while the swash eroded the upper beach face. 相似文献
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Experiments are carried out in a wave basin in order to study the swash–groundwater interaction. A set of wave gages and pressure sensors are used to monitor the free surface and groundwater dynamics. The study is based on the comparison of two selected cases which differ by the gravity and infragravity forcing conditions, the features of wave breaking in the surf zone, the presence of a standing wave attached to the beach face and the wave setup at the shoreline. Significant differences are observed in the response of the swash–groundwater system. The water table overheight appears to be controlled by the amount of infragravity energy available at the shore. Cyclic beach drainage processes can be observed when the water table is low. Significant time-averaged and time-resolved flows are observed into the sand, depending on the swash hydrodynamics. The presence of a gravity standing wave modulation attached to the shore is shown to affect swash and groundwater dynamics. Most of the pressure gradients observed under the swash zone are related to infiltration flows and are thus related to moderate increase of the sediment relative weight. 相似文献
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Low-frequency waves in the surf and swash zones on various beach slopes are discussed using numerical simulations. Simulated surface elevations of both primary waves and low-frequency waves across the surf zone were first compared with experimental data and good agreement found. Low-frequency wave characteristics are then discussed in terms of their physical nature and their relationship to the primary wave field on a series of sea bottom slopes. Unlike primary waves, low-frequency wave energy increases towards the shoreline. Low-frequency waves in the surf and swash are a function of incident waves and the sea bottom slope and hence the saturation level of the surf zone. Wave energy on a gently sloping beach is dominated by low-frequency waves while primary waves play a significant role on a steep beach. Low-frequency wave radiation from the surf zone on a given beach depends on primary wave frequency and beach slope. However, a very poor correlation was found between surf similarity parameter and low-frequency wave radiation. 相似文献
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Modelling storm impacts on beaches, dunes and barrier islands 总被引：10，自引：0，他引：10
Dano Roelvink Ad Reniers Ap van Dongeren Jaap van Thiel de Vries Robert McCall Jamie Lescinski 《Coastal Engineering》2009,56(11-12):1133-1152
A new nearshore numerical model approach to assess the natural coastal response during time-varying storm and hurricane conditions, including dune erosion, overwash and breaching, is validated with a series of analytical, laboratory and field test cases. Innovations include a non-stationary wave driver with directional spreading to account for wave-group generated surf and swash motions and an avalanching mechanism providing a smooth and robust solution for slumping of sand during dune erosion. The model performs well in different situations including dune erosion, overwash and breaching with specific emphasis on swash dynamics, avalanching and 2DH effects; these situations are all modelled using a standard set of parameter settings. The results show the importance of infragravity waves in extending the reach of the resolved processes to the dune front. The simple approach to account for slumping of the dune face by avalanching makes the model easily applicable in two dimensions and applying the same settings good results are obtained both for dune erosion and breaching. 相似文献