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1.
应用MIKE21建立胶州湾平面二维潮流模型,对青岛胶州湾大桥建设前后胶州湾内的潮流场进行数值模拟,探讨了青岛胶州湾大桥建设对周边海域的潮位、潮流、潮通量等水动力环境的影响。通过胶州湾大桥两侧的连续实测海流、潮位资料与模拟结果进行比较,可以看出两者趋势基本符合,说明该模型能够较精确地反映胶州湾大桥建设前后的潮流场分布情况。计算结果表明,大桥的建设具有一定的阻流作用并减小了过水断面,从而对周边海域的水动力环境产生一定的影响,但对胶州湾整体潮流场改变较小,影响范围限于桥位南北1.5km范围内。  相似文献   

2.
胶州湾海面溢油轨迹的数值模拟   总被引:1,自引:0,他引:1  
对胶州湾湾口两侧——团岛和薛家岛 1个月的潮位观测资料进行调和分析 ,得出湾口两侧 M2 ,S2 ,O1,K1分潮的调和常数 ,进而建立了胶州湾内的预报潮流场。考虑风场对海面溢油的影响 ,给出了预测胶州湾溢油飘移轨迹的数值模型 ,对 1 983年 1 1月 2 5日“东方大使”号油轮在中砂礁触礁后的溢油的油膜漂移轨迹进行了数值模拟 ,结果与事故后观测到的结果相符 ,说明了数值模拟的正确性  相似文献   

3.
胶州湾海面溢油轨迹的数值模拟   总被引:13,自引:0,他引:13  
对胶州湾湾口两侧--团岛和薛家岛1个月的潮位观测资料进行调和分析,得出湾口两侧M2,S2,O1,K1分潮的调和常数,进而建立了胶州湾内的预报潮流场。考虑风场对海面溢油的影响,给出了预测胶州湾溢油飘移轨迹的数值模型,对1983年11月25日“东方大使”号油轮在中砂礁触礁后的溢油的油膜漂移转变进行了数值模型,结果与事故后观测到的结果相符,说明了数值模拟的正确性。  相似文献   

4.
胶州湾潮汐潮流动边界数值模拟   总被引:11,自引:4,他引:7       下载免费PDF全文
基于普林斯顿海洋模式,通过干湿网格判别法引入潮汐潮流的漫滩过程,考虑M2,S2,K1,O1,M4和MS4六个主要分潮,建立了胶州湾潮汐潮流数值模拟和预报模型,研究了该海域潮汐潮流特征,并讨论了漫滩对潮流模拟的影响。与实测资料的对比验证表明,该模式能够对胶州湾的潮汐和潮流做出较为合理的预测。给出了胶州湾潮汐、潮流、余流等分布特征,模拟的潮流场以及余流场涡旋等现象与观测符合良好;计算了潮波能通量,从能量角度探讨了潮波的传播特性;对潮位与潮流场演变规律,以及潮能通量的分析表明,胶州湾内的潮波以驻波为主。通过数值试验发现,漫滩过程的引入对胶州湾潮流速度的模拟至关重要,不考虑漫滩过程的模式会夸大或者低估潮流流速。对于滩涂面积广阔的海域来说,潮流数值模式中考虑漫滩的影响是必要的。  相似文献   

5.
利用有限元海洋模式ADCIRC (Advanced Circulation Model),建立了高分辨率的渤黄海二维潮汐潮流数值模型,该模型以M2,S2,K1,O1等8个分潮的水位作为驱动,模拟出了该8个分潮的潮汐潮流调和常数;利用该调和常数预报的潮位和二维平均潮流与实测资料相比,符合较好;利用模拟得到的潮汐潮流调和常...  相似文献   

6.
收集了近年来鳌江口附近海域多个工程不同阶段5个潮位站的3-5年潮位实测数据和部分海流实测资料,通过对鳌江口附近海域的不同年份的水位资料进行潮汐调和常数分析,鳌江近海海域主要为半日潮区,其中M2分潮的振幅在170~193 cm;迟角在260°~280°之间,这些站的2007年、2010年、2011年调和常数分析结果相比,主要的半日分潮M2、S2、N2,全日分潮K1、O1及浅水分潮M4、MS4、及M6等分潮振幅、迟角的最大变化分别在1.8~4.4 cm和3°~7°之间。在初步掌握了鳌江口潮汐潮流特征的基础上,采用无结构的三角形网格和有限体积法的FVCOM海洋数值模型,进行模拟结果验证,计算结果与实测数据符合良好。构建重点年份建设工程合拢产生新的岸线水深的潮汐潮流场,刻画鳌江口建设工程的叠加影响。  相似文献   

7.
收集了近年来鳌江口附近海域多个工程不同阶段5个潮位站的3~5年潮位实测数据和部分海流实测资料,通过对鳌江口附近海域的不同年份的水位资料进行潮汐调和常数分析,鳌江近海海域主要为半日潮区,其中M2分潮的振幅在170 cm~193 cm;迟角在260°~280°之间,这些站的2007年、2010年、2011年调和常数分析结果相比,主要的半日分潮M2、S2、N2,全日分潮K1、O1及浅水分潮M4、MS4、及M6等分潮振幅、迟角的最大变化分别在1.8 cm~4.4 cm和3°~7°之间。在初步掌握了鳌江口潮汐潮流特征的基础上,采用无结构的三角形网格和有限体积法的FVCOM海洋数值模型,进行模拟结果验证,计算结果与实测数据符合良好。构建重点年份建设工程合拢产生新的岸线水深的潮汐潮流场,刻画鳌江口建设工程的叠加影响。  相似文献   

8.
ECOM模式在胶州湾潮流计算中的应用   总被引:17,自引:1,他引:16  
鲍献文  闫菊  赵亮  石磊 《海洋科学》1999,23(5):57-60
将ECOM模式应用于胶州湾分潮的潮汐与潮流数值模拟,结果与观测资料符合较一维潮流水平与垂直分布结构以及若干个潮致余流涡的水平分布状况。  相似文献   

9.
根据崂山头、朝连岛、灵山岛一个月的潮位资料,采用三角形网格的分步杂交方法,建立了胶州湾及邻近海域的二维变边界潮流数值模型。并模拟了大、中、小潮三种潮汛条件下的潮流场,水位场及余流场。得出了胶州湾高潮水域面积、潮间带面积,湾口累积流通量等有关参数。  相似文献   

10.
渤海海峡拉格朗日余流的数值模拟   总被引:1,自引:0,他引:1       下载免费PDF全文
本文首先用二维非线性模式对渤海海峡的M2分潮进行数值模拟,求得逐太阴时潮位和潮流场,进而导出欧拉型的潮余流,计算结果与实测资料符合良好. 在潮流模拟的基础上,对海峡中投放的标识质点的拉格朗日运动进行数值跟踪,获得典型潮时起算的拉格朗日漂移和拉格朗日余流,与欧拉余流相似,拉格朗日余流也呈北大南小之势,但二者的量值并不相同.对于确定的潮流场,欧拉余流是定常的,而拉格朗日余流却是潮位相的函数.  相似文献   

11.
By use of the hydrodynamic model,the harmonic constants of 8 principal tidal constituents(Q_1,O_1,P_1,K_1,N_2,M_2,S_2andK_2)are obtained for the East China Sea,and the harmonic constant ofS_a is calculated by two-dimensional interpolation.The calculated results agree well with the observed dataaround the sea.The harmonic constants can be used to predict the tide in the East China Sea.The cotidalcharts of the 9 tidal constituents reveal their distribution.  相似文献   

12.
选取4组不同的潮汐分潮,包括8分潮和13分潮,基于动态抗差模型对南海北部海域周边北海、海口等8个长期验潮站20年以上的日均水位序列进行分析,求取各验潮站的多年平均海面和海平面变化。结果表明,选取不同的分潮对于应用此模型求解多年平均海面和海平面变化,最大互差分别为6.1mm和0.15mm/a,差值变化在毫米级,即选取20年以上的周期序列应用动态抗差模型分析海平面时,采用8分潮模型即可满足精度要求。  相似文献   

13.
泰国湾及邻近海域潮汐潮流的数值模拟   总被引:2,自引:0,他引:2  
本文基于FVCOM(Finite-Volume Coastal Ocean Model)模式,模拟了泰国湾及其周边海域K1、O1、M2和S2四个主要分潮。采用47个验潮站实测调和常数与模拟结果进行比较,所得4个分潮的均方差分别为4.06cm、3.76cm、8.22cm和4.71cm,符合良好。根据计算结果分析了泰国湾及其周边海域的潮汐、潮流的分布特征和潮波的传播特征。数值试验表明,现有的数字水深资料(ETOPO1,ETOPO5,DBDB-V)的准确度不足以合理地模拟泰国湾潮波。  相似文献   

14.
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   

15.
Water level observations from tide stations and current observations from current-meter moorings in South San Francisco Bay (South Bay), California have been harmonically analysed. At each tide station, 13 harmonic constituents have been computed by a least-squares regression without inference. Tides in South Bay are typically mixed; there is a phase lag of approximately 1 h and an amplification of 1·5 from north to south for a mean semi-diurnal tide. Because most of the current-meter records are between 14 and 29 days, only the five most important harmonics have been solved for east-west and north-south velocity components. The eccentricity of tidal-current ellipse is generally very small, which indicates that the tidal current in South Bay is strongly bidirectional. The analyses further show that the principal direction and the magnitude of tidal current are well correlated with the basin bathymetry. Patterns of Eulerian residual circulation deduced from the current-meter data show an anticlockwise gyre to the west and a clockwise gyre to the east of the main channel in the summer months due to the prevailing westerly wind. Opposite trends have been observed during winter when the wind was variable.  相似文献   

16.
The principal characteristics of the tides are investigated by a shipborne acoustic Doppler current Profiler at a fixed station located in the Beibu Gulf from 4 to 14 April 2003. Data analysis indicates that the diurnal tidal currents dominate local current variations at the observing site. Except the barotropic M_2 constituent, four principal tides comprise both back-and-forth barotropic and baroclinic tidal currents. The baroclinic tidal ellipse parameters vary with depth, showing complicate features, rather than monotonous features being figured. For baroclinic tidal constituents, vertical modes are different to each other. Similarly, the semi-major axes of the tidal constituents vary with depth. In the lower layer, a nonlinear regression approach is used to calculate and obtain the SEMA profiles of diurnal tidal constituents. Results show that in the thin bottom boundary layer, all of the parameters vary drastically with depth, totally distinguished from the vertical profiles above.  相似文献   

17.
The characteristics of currents and tidal currents in the Andaman Sea(AS) are studied during the second half of2016 using observed data from a moored acoustic Doppler current profiler(ADCP) deployed at 8.6°N, 95.6°E.During the observation period, the mean flow is 5–10 cm/s and largely southward. The root mean square and kinetic energies of the low and high frequency flows, which are divided by a cutoff period of 5 d, are at the same level, indicating their identical importance to the total current. A power spectrum analysis shows that intraseasonal oscillations, a tidal-related semilunar month signal, a semidiurnal tidal signal and periods of 3–4 d are prominent. The barocliny of an eddy kinetic energy is stronger than the mean kinetic energy, both of which are the strongest on the bottom and the weakest at 70 m depth. Residual currents are largely southward(northward) during the summer(winter) monsoon season. Two striking peaks of the southward flow cause the 80 d period of meridional currents. The first peak is part of a large-scale circulation, which enters the AS through the northern channel and exits through the southern channel, and the second peak is part of a local vortex. The 40 d oscillation of the zonal current is forced by geostrophic variations attributed to local and equatorial remote forcing. The tidal current is dominated by semidiurnal constituents, and among these, M2 and N2 are the top two largest major axes. Moreover, astronomical tidal constituents MM and MSF are also significant. Diurnal constituents are weak and shallow water tides are ignorable. The aims are to introduce the new current data observed in the AS and to provide initial insights for the tidal and residual currents in the Andaman Sea.  相似文献   

18.
A two-dimensional hydrodynamic model application to the San Francisco Bay was performed using the Boundary-Fitted HYDROdynamic model (BFHYDRO). The model forcing functions consist of tidal elevations along the open boundary and fresh water flows from the Delta Outflow. The model-predicted surface elevations compare well with the observed surface elevations at five stations in San Francisco Bay. Mean error in the model predicted surface elevations and currents are less than 7 and 9%, respectively. Correlation coefficients for surface elevations and currents are higher than 0.94 and 0.95, respectively. The amplitudes and phases of the principal tidal constituents at 24 tidal stations in San Francisco Bay, obtained from a harmonic analysis of a 90-day simulation compare well with the observed data. The predicted amplitude and phase of the M2 tidal constituent at these stations are respectively within 8 cm and 8° of the observed data. Maximum errors in the K1 harmonic amplitudes and phases are less than 3 cm and 7° respectively. The asymmetric diurnal and semi-diurnal tidal ranges and spring and neap tidal cycles of the surface elevations and currents are well reproduced in the model at all stations.  相似文献   

19.
This part of the paper examines near-surface current data from different periods during the test mooring of the data buoy, DB1.Harmonic analyses show that variations in the major tidal constituents between each period are not significantly greater than the standard error of the measurement: the differences observed in the principal lunar semi-diurnal tide are explained partly in terms of a modulation by adjacent constituents. Unexpected forms for the quarter diurnal tidal ellipses derived from the DB1 data have been found also in independent measurements, in which a different mooring technique had been used. These are therefore unlikely to be of instrumental origin.Non-tidal energy at periods exceeding three days is shown to correlate with changes in wind and surface elevation, the correspondence between wind and current being greatest during a period of strong winds, when current at 3 m depth was 0.9% of wind speed at 8 m. The data are interpreted in favour of an Eulerian current rather than Lagrangian Stokes transport due to waves. Rectification of wave orbital velocities due to buoy motion is not detectable.In view of the overall quality of the data it is concluded that this combination of surface following buoy and long-path acoustic current meter can contribute usefully to the determination of mean near-surface currents in the open sea.  相似文献   

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