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1.
渤海三维风生-热盐-潮致Lagrange余流数值计算   总被引:9,自引:4,他引:9       下载免费PDF全文
笔者基于一种三维斜压浅海Lagrange余流的弱非线性理论,湍粘性系数的处理引进了Richardson数,利用流速分解法,把作为强迫力的潮汐、风和热盐统一在一个模型中,考虑了黄海暖流余脉和黄河径流的影响,诊断计算并获得了渤海三维风生-热盐-潮致Lagrange余环流.同时,给出了潮致Lagrange余环流、风生环流和热盐环流,并且做了比较和分析.对渤海Lagrange余环流的三个主要涡旋形成机制进行了初步的探讨.最后,用实测资料对计算结果进行了检验,显示了结果的合理性.  相似文献   

2.
渤海夏季潮致-风生-热盐环流的数值诊断计算   总被引:11,自引:5,他引:6  
基于正交曲线坐标的ECOMSED三维水动力模式,并考虑了潮汐、风和实测温盐场,诊断计算了渤海夏季三维潮致-风生-热盐环流,分析了渤海夏季潮致余流、风生和热盐环流的分布结构。结果显示,在夏季,渤海中部海区明显存在一个顺时针向的涡旋,同时渤海还存在着多个逆时针向的涡旋。通过分析和比较各个分量在总环流中的作用,认为夏季潮致余流是相对弱的;热盐环流在夏季总环流中占主要成分。  相似文献   

3.
基于有限体积方法的海洋数值模式FVCOM,计算了南黄海西部六月份潮致余流及风生环流,分析了潮致余流、初夏风生环流各自的环流结构,得出六月份该区域风生环流占主导,偏南风的作用较为显著,潮致余流相对较弱。最后将风和潮汐进行耦合计算,得出该区域初夏的环流结构,表层海水大体为由南至北的流动,说明该区域风力为主要驱动力。计算结果与流速及环流实测资料吻合较好,为进一步研究浒苔的漂移轨迹等奠定了动力基础。  相似文献   

4.
杭州湾潮致余流数值研究   总被引:7,自引:0,他引:7  
运用1959年10月-1992年5月在杭州湾250余测次海流周日连续观测资料,运用σ坐标系下的三维潮控制方程,模拟该湾的欧拉余流,进行欧拉余流产生机制的数值试验;并根据欧拉流动的数值计算结果,采用拉格朗日速度在欧拉流场的近似展开,求得水质点运动轨迹和速度。结果表明,杭州湾潮致余流的最大余流速度为46.0CM/S,惯性效应是杭州湾潮致余流产生的主要原因,杭州湾拉格朗月余流场被逆时针的大涡旋控制,表层  相似文献   

5.
东中国海潮余流自适应数值模拟   总被引:4,自引:2,他引:4  
以自适应数值模型首次计算整个东中国海三维 M2 分潮潮致 Euler余流、Stokes漂流和L agrange余流 ,并分析各海区 L agrange余流的特征。渤海 M2 分潮致 L agrange余流在整个海域基本形成一个大的逆时针环流系统 ;辽东湾有一个逆时针流环。在黄海 ,潮致余流也是黄海环流的重要组成部分。在东海的东北部 ,潮致余流有强化对马暖流的作用 ;在台湾北部海域 ,潮余流对台湾暖流有强化作用。在近海海域 ,由于复杂地形的作用 ,潮流非线性作用加强 ,潮余流的量值有较明显的增加。计算结果表明 :在浅水区域 ,Stokes漂流较大 ,Euler余流与 Lagrange余流差别显著  相似文献   

6.
洋浦是典型的日潮区,潮型判别系数是7.32;最大潮流流速都出现在涨潮的北向流中,最大潮流速度为70cm/s.余流的表、中、底30d平均流向依次为188(°)、153(°)和95(°).表、中、底30d平均余流流速值依次为8.7、8.5和4.1cm/s.冬季余流的形成,主要受北部湾风生环流控制.  相似文献   

7.
东海沿岸潮致上升流的数值模拟   总被引:3,自引:0,他引:3  
卫星照片显示东海沿岸存在一条狭长的低温水带,这是上升流将外海深层低温海水带到近岸表层所造成的现象。本文从潮汐因素探讨上升流产生的原因。对东海沿岸海域M2分潮进行三维潮流数值计算,得出的各层水平余流和垂直余流表明,由于潮汐非线性效应和海底地形的影响,能够在中国东海沿岸产生一条狭长的上升流带。此结果与卫星照片显示的海面低温水域的范围基本一致。此外还计算了在不同风速、风向作用下产生的风生上升流,并与潮致上升流进行了比较  相似文献   

8.
渤海冬季三维环流数值模拟   总被引:1,自引:2,他引:1  
基于冯士笮所给出的一种浅海环流模型,采用数值方法,对渤海冬季进行环流的数值模拟,给出了冬季三维风生环流和正压环流(含潮余流)。分析了潮致Lagrange余流对冬季环流的贡献及黄海暖流余脉对渤海冬季环流的影响。最后对风生环流和正压环流的特征进行了分析和讨论。  相似文献   

9.
渤、黄、东海夏季环流的三维斜压模型   总被引:10,自引:0,他引:10  
基于拉格朗日时均观点描述环流,建立起潮流与准定常流共同占优势系统中的陆浅海环流模型,并诊断计算了夏季渤、黄、东海的三维环流图。模拟结果较好地再现了渤、黄、东海主要流系的特征。对照冬季结果,对渤、黄、东海环流的季节变化做了阐述。从环流垂向分量的分布图上,可发现渐闽近海、长江口外存在较明显的上升流区。另外,对夏季渤、黄、东海的热盐环流和潮致余流分别进行了模拟,发现它们均能在黄海构成一逆时针向的五流系统,这对形成和维持夏季黄海冷水团的存在有重要作用。热盐环流的模拟结果表明,黄海冷水团环流含有“热成流”的成分;通过Lagrange余流的计算发现环绕黄河冷水团的环流还含有“潮成流”的成分。  相似文献   

10.
为了研究渤海湾潮致余流,运用Mike21模拟了渤海湾潮流场,揭示出潮波运动的规律,得到渤海湾的潮流场,在涨潮时最大流速为1.4m/s,落潮时最大流速为1.12m/s。根据欧拉余流的定义计算了潮致欧拉余流场,其最大流速为0.2m/s,中值为0.005m/s,在渤海湾北部区域和南部东营附近存在环状结构。在渤海湾不同位置释放自由粒子,通过粒子的运移路径发现渤海湾拉格朗日余流呈现双环结构。运用欧拉方法和拉格朗日方法分析渤海湾潮致余流场,阐明了渤海湾潮致余流的精细结构,可为渤海湾营养盐、沉积物或者污染物质的长期输送以及浮游生物、鱼卵等的迁移和分布规律等提供动力学基础。  相似文献   

11.
北部湾三维风生流及密度流模拟   总被引:16,自引:0,他引:16  
将Casulli差分格式引入三维物理海洋模型计算,模拟了北部湾风生流及密度流。模拟结果表明,夏季西南季风在北部湾导致一个顺时针环流,夏季海水密度梯度导致一个逆时针方向的环流,密度流明显强于风生流;冬季东北寒潮导致一个逆时针环流。模拟结果不支持北部湾夏季为一顺时针环流、冬季为逆时针环流的传统结论,而支持终年为逆时针环流的观点。  相似文献   

12.
On the basis of a three-dimensional weakly nonliear theory of Lagrangian residual current in the Baroclinic shallow seas, a diagnostic numerical calculation of wind-driven, thermohaline and tide-induced Lagrangian residual current in the Bohai Sea is made. The model involves the Richardson number in the eddy viscosity coefficient, wind, thcrmolialine and tidal effects in the focing terms. The runoff of the Huanghe River and a part of the Huanghai Warm Water coming from the Huanghai Sea through the Bohai Sea Strait is also considered. The velocity-splitting method is adopted. The wind-driven circu lation, thermohaline circulation and the tide-induced Lagrangian residual circulation are also obtained individually and analysed. The dynamics of the three main eddies in the Lagrangian mean circulation is discussed. Finally, the numerical result is partly verified with the observed data.  相似文献   

13.
The Beibu Gulf circulation plays an imPOrtant role in the long--term water rnass transportinside the gulf. It is also closely related to the Guangxi untal water mass transport and self-purification. Hence, it is of practical imPOrtance to study the circulation in the gUlf. The cir-culation in the gUlf is very comlicated, and is rnainly gOverned by wind, water density gradi-ent, the current outside the gulf and the bathpoetry. In spring, a cold water rnass generatesln the center of the gulf…  相似文献   

14.
A Study on Residual Flow in the Gulf of Tongking   总被引:2,自引:0,他引:2  
On the basis of observations of water temperature, salinity and wind during winter (December to following February) and summer (June to August) in the Gulf of Tongking, a robust diagnostic three-dimensional model has established that reveals the seasonal variation in residual flow, including wind-driven current, density-driven current and tide-induced residual current. It is shown that in the Gulf of Tongking the wind-driven current plays the most important role in the seasonal variation of residual flow field. Due to strong NE monsoon (9 m/s) during winter the residual flow (reaches 30 cm/s) is stronger than that in summer. At the surface the residual flow direction during winter is basically westward or southwestward, while during summer it is almost reversed.  相似文献   

15.
渤海的潮汐余流   总被引:9,自引:0,他引:9  
本文采用二维非线性潮波微分方程,依据目前的海图对渤海M_2、S_2、K_1、O_1的潮汐余流进行了数值计算,并进一步计算了由这4个分潮组成的总潮汐余流。计算表明,渤海以M_2的潮汐余流占主要地位,S_2、K_1、O_1的潮汐余流具有大约相同的量值。但是,它们比M_2小一个量级。为探讨渤海潮汐余流自30年代以来的变化情况,本文还依据30年代的渤海海图和设想数十年后渤海的海图,对M_2进行数值计算,求得这二个时代的M_2潮汐余流。结果表明,自30年代以来,莱州湾的潮汐余流发生了很大的变化。  相似文献   

16.
It is of some limitations to analyse residual currents by means of the 25 h anchored current measurements. On the basis of the drift tracking and the mooring system data, here, analyses have been done aiming at the structural characteristics and the dynamical mechanisms of the frontal residual current field of the Hangzhou Bay. Especially a theoritical model is given focusing on the frontal density-driven currents. The results indicate that there exists obviously the upper-layer front-driven flow along the orientation of the front during neap tides in the research area of the Hangzhou Bay. But the flow is restrained by the strong vortical viscosity during spring tides. In the lower layer, the effect of the front is little and the subtidal movements are dominated by the tide-induced residual currents. In addition, the influences of wind forcing to the residual current field are also suggested to be important.  相似文献   

17.
Hydrodynamic model application to Buzzards Bay is performed using a three-dimensional Boundary-fitted Hydrodynamic model in this study. The model is forced with observed tidal harmonic constants along the open boundaries and winds on the surface. The main focus of the present study is to model the detailed wind and tide-induced circulation in Buzzards Bay. The observed surface elevations and currents given in [Butman, B., Signell, R., Shoukimas, P., Beardsley, R.C., 1988. Current Observations in Buzzards Bay, 1982–1986. Open File Report 88-5. United States Geological Survey] and the tide and current harmonics given in [Signell, R.P., 1987. Tide- and Wind-forced Currents in Buzzards Bay, Massachusetts. Technical Report WH-87-15. Woods Hole Oceanographic Institution, Woods Hole, Massachusetts] are used to validate the model predictions. The calibrated model is then used to study the relative contributions of tidal and wind forcing on the instantaneous and residual circulation in Buzzards Bay. The amplitudes and phases of the principal tidal constituents at 10 tidal stations in Buzzards Bay obtained from a harmonic analysis of a 60-day simulation compare well with the observed data. The predicted amplitude and phase of the M2 tidal constituent of surface elevations at these stations are, respectively, within 4 cm and 5° of the observed data. The errors in the model-predicted M2 harmonic principal current speeds are less than 6 cm/s, and the principal current directions and phases are within 14° of the observations. The observed surface elevations and currents given in [Butman, B., Signell, R., Shoukimas, P., Beardsley, R.C., 1988. Current Observations in Buzzards Bay, 1982–1986. Open File Report 88-5. United States Geological Survey] are used to validate the model-predicted low-frequency surface elevations and currents. The model predictions in low-frequency surface elevations at Woods Hole closely follow the trends seen in the observations with a correlation coefficient of 0.735, but fail to capture some of the peak surges seen in the observations. The model-predicted low-frequency currents in the east–west direction at stations in Buzzards Bay compare well with the observations with the correlation coefficient exceeding 0.811 and the model capturing the trends seen in the observations, for the most part. However, the model-predicted north–south velocities does not compare well with the observations. The model-predictions agree with the observations that the tidal currents in Vineyard Sound lagged the currents in Buzzards Bay by more than 3 h. The interaction of wind stress with large bathymetric gradients was shown to cause many vortices in Buzzards Bay, as seen from the model predictions. Model simulations show that the winds play a more dominant role than the tides in the generation of the barotropic residual currents in Buzzards Bay, while the model-predicted tide-induced residual current was seen to be small.  相似文献   

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