共查询到19条相似文献,搜索用时 93 毫秒
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计算方法如图(3)所示,石臼港面临广阔的海域,曲线表示岸线,A、B、C、D为岸线格网点。二期工程拟从A点至E点修建码头和防波堤。建成后港内X方向最大距离为5100米,Y方向在湾口处为2600米。三期工程如图(5)所示,湾口宽为500米。二、三期工程建成后,港内的潮流流场必将发生巨大的变化。建港前预知建港后的潮流 相似文献
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大鹏湾潮流场的数值模拟 总被引:1,自引:1,他引:1
本文根据描述潮流运动变化的连续方程和运动方程,用ADI方法建立差分方程,对大鹏湾潮流场进行了数值模拟;从而根据数值模拟结果和实测结果,对大鹏湾的潮流和潮汐余流等进行了讨论。 相似文献
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将三维浅海流体动力学的流速分解模型简化为二维潮模型。在Ara-Kawa-B网格上,对黄茅海的潮位和潮流进行数值模拟。结果表明,黄茅海是一个往复流海区,与实际吻合较好。 相似文献
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为了能够精确地拟合天然水域不规则的水陆边界,并能保持有限差分数值计算在矩形网格中进行,本文利用Thompson的数值网格生成技术,在长江口南支七丫口至横沙河段设计了一个椭圆型边界拟合坐标系,并在这个坐标系下建立了平面二维潮流数学模型。通过数值求解此数学模型,实现了计算区域内现状潮流的一个数值模拟,模拟结果表明,模式的设计是成功的。 相似文献
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北部湾潮汐潮流的数值模拟 总被引:1,自引:0,他引:1
基于正交曲线坐标的ECOMSED三维水动力模式,对北部湾的潮汐潮流进行数值模拟。选用不同的海底摩擦系数、海底粗糙度系数以及水平湍流摩擦系数进行数值试验。试验结果表明,当海底摩擦系数取2×10-3~3×10-3,海底粗糙度系数取1×10-3~2×10-3m,而水平湍流摩擦系数取1×102~5×103m2/s时,模拟所得潮汐、潮流结果与实测数据吻合较好;并由此对北部湾的潮汐、潮流和潮余流等特征进行了分析。还给出了垂直湍流黏滞系数呈抛物型的分布特征。对该海域的水动力状况有了进一步的了解,为该海域的环境保护规划提供了科学依据。 相似文献
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厦门湾潮流场的数值模拟 总被引:3,自引:1,他引:3
本文依据二维长波方程,用ADI方法建立差分方程,计算了厦门湾附近海域的半日潮和全日潮,并考虑了计算域西部九龙江的径流对该海域流场的影响,得到瑟实际观测符合良好的结果;从而根据数值模拟实测结果,对厦门湾的潮汐和潮流等进行了讨论。 相似文献
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The spatial and temporal variability of tidal mixing in Bohai Sea is studied using a numerical approach. In calculating tidal mixing, accurate barotropic tidal current is obtained via a harmonic analysis package utilizing the simulated current output from a high-resolution regional ocean model. And a “small-scale” roughness map is adopted to describe the detailed topographic features of Bohai Sea. It is shown that the tidal mixing estimated in Bohai Sea is much higher than the level of global background, and fluctuates considerably at some regions within a single day. In Liaodong Bay, Bohai Bay and Bohai Strait, the mixing varies greatly, with the peak value of O (10?2) m2 s?1. The order of magnitude of mixing in Laizhou Bay is about O (10?5~10?3) m2 s?1. Mixing with background level of O (10?5) m2 s?1 only appears in central area. Result also shows that rough topography plays relatively a more important role than tidal current in enhancing diapycnal mixing in Bohai Sea. The distributions of tidal mixing in selected sections reveal that the vertical stratification in Bohai Sea is not obvious, generally renders a barotropic structure. 相似文献
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利用FVCOM海洋数值模式计算了印尼近海的M2,S2,K1,O1分潮的分布,计算范围从20°S~20°N,90°~150°E,计算网格分辨率在印尼海域岛屿平均为1/12度,在大陆边界平均为1/5度,在开边界平均为1/2度.计算结果与104个TOPEX/Poseidon卫星高度计交叉点数据和79个验潮站数据进行比较,符合良好;与高度计交叉点比较,M2分潮振幅的均方根差为6 cm,迟角为7°;S2分潮的振幅偏差为3 cm,迟角偏差为8°;K1分潮振幅的偏差为6 cm,迟角偏差为10°;O1分潮振幅偏差为3 cm,迟角偏差为10°.根据计算结果给出了4个分潮的潮汐、潮流、潮余流和潮能通量密度分布图. 相似文献
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物理模拟较大海域的环境动力场是物理模型试验的一个发展方向,也是近海环境治理的有效研究手段。对具有较大尺度海域的模拟需要考虑地转缺失的影响。从潮流基本控制方程出发,通过对方程的无因次化,给出评价柯氏力作用大小的方法,并就中国典型的海湾进行尺度分析,量化物理模拟时因地转缺失引起的偏差程度,讨论在这些海域是否可以付诸物理模型试验。同时,还导出了潮流泥沙试验和潮流污染物扩散试验的相似比尺关系。 相似文献
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- Based on field wave data, an empirical formula of wave envelope spectrum is given in this paper. Then the methods of both numerical and physical simulation of sea wave groups with the given spectrum and groupiness parameters are suggested. 相似文献
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Corrected Formula of Bed Resistance Coefficient for Plane Numerical Simulation of Tidal Current 总被引:4,自引:0,他引:4
By means of a logarithm law for the velocity profile,a corrected formula of bed resistancecoefficient,which involves many factors such as gradient of still water depth,variation of surfaceelevation,flow direction,and so on,is derived from the 3D governing equations of tidal current by aver-aging over the whole water depth.Theoretical analysis and application have shown that the 2D plane tidalcurrent numerical model would be more reasonable and could be applied to steep bottom topographywhen the corrected bed resistance coefficient is used,therefore the results of reproduction simulation andengineering calculation would be more scientific and reasonable. 相似文献
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SHI Fengyan DING Pingxing KONG Yazhen
Associate Professor State Key Laboratory of Estuarine Coastal Research East China Normal University Shanghai P. R. China.
Professor State Key Laboratory of Estuarine Coastal Research East China Normal University Shanghai P. R. China.
Senior Engineer State Key Laboratory of Estuarine Coastal Research East China Normal University Shanghai P. R. China. 《中国海洋工程》1999,(2)
Fine grids with small spacing in boundary-fitted coordinates are normally used to treat thecomputation of fluid dynamics for estuarine areas and tidal flats.However,the adoption of Cartesian com-ponents of velocity vectors in this kind of non-orthogonal coordinates will definitely result in a diffculty insolving implicitly the transformed momentum equations,and also complicate the wet-dry point judgementused for flood areas.To solve this problem,equations in terms of generalized contravariant velocityvectors in curvilinear coordinates are derived in the present study,by virtue of which,anAlternative-Direction-Implicit numerical scheme in non-orthogonal grids would then be easily obtained,and wet-dry point judgement would as well be largely simplified.A comparison is made between the explic-it scheme and implicit scheme,showing that the present model is accurate and numerically stable for com-putations of fluid dynamics for estuarine areas and tidal flats. 相似文献