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1.
黄海海浪季节变化的数值模拟研究   总被引:3,自引:2,他引:1  
陈国光  翟方国  李培良  刘晓 《海洋科学》2016,40(11):155-168
利用第三代海浪数值模式SWAN,研究了黄海海浪有效波高的季节变化特征及相关的物理过程。结果表明,在黄海的大部分区域,混合浪有效波高的最大值出现在冬季,而最小值则基本出现在夏季。北黄海北部和山东半岛南岸的近海海域呈现稍微不同的季节变化,有效波高的最大值出现在春季。全年4个季节中混合浪有效波高的空间分布基本一致:均在济州岛西南最大,沿黄海中部区域向北和由中部区域向近岸区域逐渐减小。黄海海浪为风浪占主,涌浪有效波高远小于风浪有效波高。在黄海的大部分区域,白冠耗散和四波非线性相互作用对黄海海浪的季节变化均至关重要;对于外海区域,四波非线性相互作用更为重要,而对于近海区域,白冠耗散则影响更大。本研究旨在研究黄海海浪的季节变化特征及其物理过程,为进一步探讨该海域海浪在其他时间尺度上的变异特征和动力学过程提供研究基础。  相似文献   

2.
北印度洋-南海海域海浪场、风场的年际变化特征分析   总被引:3,自引:0,他引:3  
利用1957年9月~2002年8月共45年的逐6小时ERA40 10 m风场,驱动WAVEWATCHⅢ海浪模式,得出北印度洋-南海海域3小时一次,分辨率为0.5°×0.5°的海浪场;对上述海浪场和对应风场进行EOF分析,讨论它们的年际变化的特征。研究结果指出:亚丁湾以东洋面、孟加拉湾和南海都存在海浪和风速场的高值变化中心,尤其是亚丁湾以东洋面风力最强,有效波高最高;赤道印度洋中东部有效波高为高值区可能是南印度洋西风带产生的涌浪向北传播引起的;北印度洋-南海海域海面风速和有效波高呈线性增强趋势,海面风速还存在3年左右的周期变化现象。  相似文献   

3.
基于ECMWF的ERA-interim37a的风场及海浪场再分析资料,探讨了南海海域波浪的时空分布特征,主要分析了波浪场和风场的空间分布、季节特征以及4个海域(南沙、西沙、中沙、东沙)波高与周期的联合分布以及南海波高的长期变化趋势。结果表明:南海海域的有效波高大值区呈东北-西南走向,且具有明显季节性变化特征,波高与风速以及波向与风向整体相关性较好;有效波高和波周期有良好的对应关系,不同区域波高与周期联合分布相近。1979—2015年期间,南海大部分海域的有效波高呈逐年递增趋势,其量值约为0.2~0.8 cm/yr。本文的研究成果,对南海远洋运输、海洋工程设计、岛礁建设及海洋能开发与利用等有着重要的参考价值。  相似文献   

4.
东中国海及毗邻海域海面风场季节及年际变化特征分析   总被引:5,自引:0,他引:5  
本文基于美国Remote Sensing Systems公司提供的QuickScat海面风场产品,空间分辨率为0.25°×0.25°的月平均资料,进行了两种经验正交函数分解(EOF),以此分析研究中国近海(渤海、黄海、东海)以及台湾以东、以南洋面海面风场的季节变化和年际变化特征。研究发现:(1)季节变化是东中国海海表面风速变化的最主要特征,其变化占总变化方差的70.9%,黑潮的季节变化,通过海气交换影响其流经海域局地风场;(2)东中国海及毗邻海域海表面风速变化与太平洋年际变化以及热带风暴爆发有关,东中国海海表面风速年际变化显著的周期为1.5年和3.1年;(3)东中国海海域近年来整体上海表风速处于增大的趋势中,风速增大最大的区域出现在台湾东侧海域黑潮流经区域,最大增速在0.025 m/s/a以上。  相似文献   

5.
黄渤海海域波浪时空变化特征分析   总被引:1,自引:0,他引:1  
本文利用欧洲中期预报中心(ECMWF)第五代再分析数据集(ECMWF Reanalysis v5 ERA5,ERA5),对中国黄渤海海域2000-2019年的波浪进行了统计分析。得到如下的结论:1.黄渤海海区波浪具有明显的季节性,渤海区域有效波高呈现出周边小,中间大的特点;黄海海域有效波高Hs呈现由南向北降低的趋势;研究区域冬季有效波高均值大于其他季节。2.平均周期T的季节分布类似于有效波高的季节均值分布。渤海仅秋冬季T的均值存在大于4s的区域;黄海海域T的季节分布也呈现由南向北递减的趋势,其中长江口外海区域秋冬季T的季节均值可达6s。3.有效波高距平场EOF分解结果显示,第一模态表明了波浪变化具有明显的季节性特征;第二模态反映了季风的季节转换对有效波高的影响;第三模态代表的可能是地形的变化对有效波高变化的影响。4.代表点统计结果显示:整个渤海地区的常浪向为 NNE~NE,强浪向以 NE和 NNE 为主;黄海海域的常浪向为SSE-SE向,强浪向以 N和 SSE 为主。  相似文献   

6.
本文利用第三代海浪模式(WAVEWATCH III)分析了2002-2011年太平洋风速和海浪场的时空变化特征。首先,使用浮标观测数据对模式模拟的有效波高结果进行验证。结果表明模式可以有效地后报太平洋的有效波高。模式偏差较大的区域为中低纬度地区。随后将太平洋分为多个子区域,分别讨论了其风速和有效波高的时空变化特征。多年平均太平洋风速和有效波高存在类似的纬向分布特征,各子区域之间风速和有效波高的季节变化存在差别。模式刻画的太平洋有效波高年际变化最大的区域为南半球中高纬区域。进一步,我们研究了波浪能量的输入与耗散。相应的源函数项的各区域平均值显示了量化的表面波的变化。最后,对日平均的风速与有效波高值进行功率谱分析寻找序列的显著周期。结果表明有效波高时间变化对应的频谱和风速谱具有一定的差异。  相似文献   

7.
以CCMP(Cross-Calibrated,Multi-Platform)风场为驱动场,分别驱动目前国际先进的第三代海浪模式WW3(WAVEWATCH-III)、SWAN(Simulating WAves Nearshore),对2011年3月发生在中国海的一次强冷空气所致的海浪场进行数值模拟,就冷空气海浪场的特征进行分析,并对比分析两个海浪模式的模拟效果,以期可为防灾减灾提供参考。结果表明:(1)以CCMP风场分别驱动WW3、SWAN海浪模式,可以较好地模拟发生在东中国海的冷空气海浪场过程,两个模式模拟的有效波高都具有较高精度,SWAN模拟的有效波高明显小于观测值和WW3模式的模拟值。(2)冷空气给中国海带来了明显的大风、大浪过程。整个冷空气期间,波向与风向保持了较好的一致性,且向岸效应比较明显;波高与风速的分布特征也保持了较好的一致性,海浪以风浪为主导。(3)冷空气进入渤海,相伴着出现了大风过程,但由于海域狭小,大风范围较小,大风中心的风速仅12 m/s左右,相应波高也在1.0 m左右。冷空气南下进入黄海中部时,黄海中南部大范围海域的风速在16 m/s以上,相应区域的波高在4.5 m以上,高值中心可达5.0 m以上,波向和风向都以北-东北向为主。冷空气南下行进至南海北部海域时,强度大为减弱,风速的和波高的相对大值区分布于台湾岛周边海域,尤其是台湾海峡、吕宋海峡、东沙群岛附近海域。  相似文献   

8.
全球再分析数据集已成为研究气候规律和数值模拟的重要工具,其中海面风场数据集是波浪模拟的重要资料,风场资料的准确性是影响海浪要素模拟结果的关键因素,不同的海面风场资料在中国各个海域的适用性具有不确定性。利用黄海、东海海域的12个观测点,选取了2006—2018年间的11场台风进行对比,验证了ERA5和NCEP风场在台风期间与常海况下的风速;模拟了中国近海海域的波浪场,与范围内15个测站的有效波高及谱峰周期进行了对比验证;分析了ERA5和NCEP风场在黄海、东海波浪模拟的适用性。主要结果如下:(1)风场质量是造成台风浪模拟误差的主要原因之一,研究区域内ERA5风场在台风期间的风速大小与实测资料具有较高一致性;长江口邻近海域内,ERA5风速相关性在0.8以上;江苏海域内,ERA5风速相关性在0.9以上;(2)分别采用ERA5和NCEP再分析风场资料作为驱动风场输入Mike21 SW模型,较好地模拟了黄海、东海海域在不同海况下的波浪变化情况;在江苏海域,ERA5资料模拟波高值与浮标测站观测波高资料相关性超过0.85,平均绝对误差不超过0.2 m;(3)两种风场在江苏海域、长江口及其邻海的适用性比黄海北部更好。结果表明,NCEP和ERA5在中国近海海域波浪模拟的适用性有差异,在江苏海域、长江口及其邻海,基于ERA5的数值模拟结果相对于NCEP模拟结果精度提高。  相似文献   

9.
1957~2002年南海—北印度洋海浪场波候特征分析   总被引:2,自引:0,他引:2  
郑崇伟  李训强  潘静 《台湾海峡》2012,31(3):317-323
利用ERA-40海表10 m风场驱动第三代海浪数值模式WAVEWATCH-Ⅲ,得到南海—北印度洋1957年9月至2002年8月的海浪场,并分析其波候(风候)特征.研究发现如下主要特征:(1)该海域的波高波向、风速风向受季风影响显著;(2)北印度洋大部分海域的海表风速呈显著性逐年线性递增趋势,大约0.01~0.02 m/(s·a),南海线性递增的区域则较少,有效波高呈显著性逐年线性递增的区域主要集中在低纬度中东印度洋(约0.003~0.006 m/a)、索马里附近海域(大约0.002~0.005 m/a)、南海大部分海域(约0.002~0.004 m/a),线性递减的区域主要集中在孟加拉湾海域(约-0.002 m/a);(3)Nino3指数与南海—北印度洋的海表风场、浪场存在密切的关系;(4)南海—北印度洋的海表风速与有效波高存在5.2a左右的共同周期,南海的海表风速、有效波高还存在2.0a左右的共同周期,北印度洋的海表风速、有效波高还存在26.0a的长周期震荡.  相似文献   

10.
基于ERA-Interim再分析资料,统计分析了南沙海域的风场、海浪场的时空特征,并进一步研究了风浪成长关系,建立了适用于南沙海域的风浪模型。月平均场分析结果表明:在季风期,南沙海域的月平均有效波高与风场的时空分布特征有良好的对应关系,位于中南半岛的东南部存在一个风速和有效波高的大值中心,冬季强于夏季,中心位置随季节转换稍向下风向移动。频率分析结果表明:南沙海域全年以4级以内风力和3级以内海浪出现的频率最高,6级以上大风和5级以上海浪主要出现在冬季风期间;全年最大风速和浪高出现在10、11月,最大风速达到8级,最大有效波高可达6级,但频率非常小;整个海域风速和浪高最小的时期是4—5月。  相似文献   

11.
The seasonal variability of the significant wave height(SWH) in the South China Sea(SCS) is investigated using the most up-to-date gridded daily altimeter data for the period of September 2009 to August 2015. The results indicate that the SWH shows a uniform seasonal variation in the whole SCS, with its maxima occurring in December/January and minima in May. Throughout the year, the SWH in the SCS is the largest around Luzon Strait(LS) and then gradually decreases southward across the basin. The surface wind speed has a similar seasonal variation, but with different spatial distributions in most months of the year. Further analysis indicates that the observed SWH variations are dominated by swell. The wind sea height, however, is much smaller. It is the the largest in two regions southwest of Taiwan Island and southeast of Vietnam Coast during the northeasterly monsoon, while the largest in the central/southern SCS during the southwesterly monsoon. The extreme wave condition also experiences a significant seasonal variation. In most regions of the northern and central SCS, the maxima of the 99 th percentile SWH that are larger than the SWH theoretically calculated with the wind speed for the fully developed seas mainly appear in August–November, closely related to strong tropical cyclone activities.Compared with previous studies, it is also implied that the wave climate in the Pacific Ocean plays an important role in the wave climate variations in the SCS.  相似文献   

12.
全球有效波高和风速的时空变化及相关关系研究   总被引:2,自引:1,他引:1  
The climatology of significant wave height(SWH) and sea surface wind speed are matters of concern in the fields of both meteorology and oceanography because they are very important parameters for planning offshore structures and ship routings. The TOPEX/Poseidon altimeter, which collected data for about 13 years from September 1992 to October 2005, has measured SWHs and surface wind speeds over most of the world's oceans. In this paper, a study of the global spatiotemporal distributions and variations of SWH and sea surface wind speed was conducted using the TOPEX/Poseidon altimeter data set. The range and characteristics of the variations were analyzed quantitatively for the Pacific, Atlantic, and Indian oceans. Areas of rough waves and strong sea surface winds were localized precisely, and the correlation between SWH and sea surface wind speed analyzed.  相似文献   

13.
基于长时间的FRA-JCOPE数据,本文着重对渤海海峡水交换的多时间尺度变化特征进行了分析。通过分析认为,渤海海峡水交换具有明显的季节(360天和180天周期)、季节内(120天周期)和年际变化特征,且空间分布呈现较为明显的“南出北进”特点。360天季节变化特征表现为夏强冬弱,局地风场、海峡两侧海表高度梯度、陆地径流的季节变化对其具有重要影响;180天周期的季节变化和120天周期季节内变化信号与局地风场关系不大,主要受到海峡两侧海表高度梯度的调制。同时,渤海海峡水交换受1997—1998年ENSO影响较为显著:正常年份时,渤海海峡水交换流入、流出量基本相当,但当1997—1998年ENSO显著年份时,流出量略大于流入量,这是由于黄渤海环流增强,进而导致渤海海峡水交换增强造成的。  相似文献   

14.
WWATCH模式模拟南海海浪场的结果分析   总被引:25,自引:3,他引:25       下载免费PDF全文
利用美国NOAA/NCEP环境模拟中心海洋模拟小组近年新开发的一个准业务化的海浪数值模式WAVEWATCH Ⅲ(以下简称WWATCH),以每天4次的NOAA/NCEP再分析风场资料为输入,模拟了1996年的南海海域的海面风浪场,通过分析TOPEX/Poseidon(以下简称T/P)高度计的上升和下降轨道在南海海域的交叉点位置处的风、浪观测资料与NCEP风场和WWATCH模式模拟的有效波高大小,可以看出,NCEP风场基本与T/P高度计的风速观测结果一致,相应的模式模拟的有效波高也基本与卫星高度计的有效波高观测结果相一致,但从空间上看,在计算区域中心附近海域的结果一致性较好,靠近计算边界附近海域的结果相对较差,但这种因边界而影响模拟结果的范围很有限;从时间上看,冬季风期间的结果一致性较好,而夏季风期间的结果偏小的趋势明显,并且这种偏小主要出现在夏季风期间的极小风速值附近。  相似文献   

15.
In this paper, interannual variations of the ocean dynamic height over the tropical Pacific are diagnosed using three-dimensional temperature and salinity fields from Argo profiles, with a focus on the...  相似文献   

16.
南海海面温度的年际模态及其与季风强迫的关系   总被引:1,自引:0,他引:1  
通过对COADS和OISST海洋气象资料的分析,以南海的海面温度异常(SSTA)为指示因子,在研究年际尺度上的南海与大尺度ENSO关系的基础上,进一步探讨了季风强迫下Ekman抽吸对SSTA年际变化的贡献。研究发现,南海SSTA滞后5个月时与:Nifio 3的SSTA相关系数最大,且其年际变化依方差贡献大小,分别有42.7月、25.6月及36.6个月的周期,这3个年际模态基本上能够描述海面温度的年际变异,为南海在大尺度ENSO背景下存在区域响应提供了重要的证据;应用Krause—Turner混合层温度方程对南海异常暖事件的研究表明,除了经向风应力异常,Ekman抽吸也是影响SSTA年际变异的主要因素,在某些异常年份甚至是主导因素,为南海SSTA年际变化的研究提供了重要的补充。  相似文献   

17.
Thirteen years (1998–2010) of satellite-measured chlorophyll a are used to establish spatial patterns in climatological phytoplankton biomass seasonality across the California Current System (CCS) and its interannual variability. Multivariate clustering based on the shape of the local climatological seasonal cycle divides the study area into four groups: two with spring-summer maxima representing the northern and southern coastal upwelling zones, one with a summer minimum offshore in mid-latitudes and a fourth with very weak seasonality in between. Multivariate clustering on the seasonal cycles from all 13 years produces the same four seasonal cycle types and provides a view of the interannual variability in seasonal biogeography. Over the study period these seasonal cycles generally appear in similar locations as the climatological clusters. However, considerable interannual variability in the geography of the seasonal cycles is evident across the CCS, the most spatially extensive of which are associated with the 1997–1999 El Niño-Southern Oscillation (ENSO) signal and the 2005 delayed spring transition off the Oregon and northern and central California coasts. We quantify linear trends over the study period in the seasonal timing of the two seasonal cycles that represent the biologically productive coastal upwelling zones using four different metrics of phenology. In the northern upwelling region, the date of the spring maximum is delaying (1.34 days yr−1) and the central tendency of the summer elevated chlorophyll period is advancing (0.63 days yr−1). In the southern coastal upwelling region, both the initiation and cessation of the spring maximum are delaying (1.78 days yr−1 and 2.44 days yr−1, respectively) and the peak is increasing in duration over the study period. Connections between observed interannual shifts in phytoplankton seasonality and physical forcing, expressed as either basin-scale climate signals or local forcing, show phytoplankton seasonality in the CCS to be influenced by changes in the seasonality of the wind mixing power offshore, coastal upwelling in the near-shore regions and basin-scale signals such as ENSO across the study area.  相似文献   

18.
Seasonal and interannual variability of the pressure field and indices of the North Atlantic atmosphere zonal circulation are analysed using historical (1894–1988) observations. It is shown that fluctuations of the index of North Atlantic oscillations (NAO) and that of the eastward transport give evidence of the interannual fluctuations with the typical time scale being 2–7 years. It is shown that the magnitude of interannual NAO index variability exceeds the typical magnitude of seasonal variations, particularly in winter. The time scale of NAO index variations and eastward transport coincides with the typicalEl Niño-southern oscillations (ENSO) temporal scale. The amplitudes of the annual, semi-annual harmonics, and high-frequency fluctuations of the NAO index increase during a typical ENSO event at least by a factor of 2.Translated by V. Puchkin.  相似文献   

19.
Tropical Pacific interannual variability is examined in nine state-of-the-art coupled climate models, and compared with observations and ocean analyses data sets, the primary focus being on the spatial structure and spectral characteristics of El Niño-Southern Oscillation (ENSO). The spatial patterns of interannual sea surface temperature (SST) anomalies from the coupled models are characterized by maximum variations displaced from the coast of South America, and generally extending too far west with respect to observations. Thermocline variability is characterized by dominant modes that are qualitatively similar in all the models, and consistent with the “recharge oscillator” paradigm for ENSO. The meridional scale of the thermocline depth anomalies is generally narrower than observed, a result that can be related to the pattern of zonal wind stress perturbations in the central-western equatorial Pacific. The wind stress response to eastern equatorial Pacific SST anomalies in the models is narrower and displaced further west than observed. The meridional scale of the wind stress can affect the amount of warm water involved in the recharge/discharge of the equatorial thermocline, while the longitudinal location of the wind stress anomalies can influence the advection of the mean zonal temperature gradient by the anomalous zonal currents, a process that may favor the growth and longer duration of ENSO events when the wind stress perturbations are displaced eastwards. Thus, both discrepancies of the wind stress anomaly patterns in the coupled models with respect to observations (narrow meridional extent, and westward displacement along the equator) may be responsible for the ENSO timescale being shorter in the models than in observations. The examination of the leading advective processes in the SST tendency equation indicates that vertical advection of temperature anomalies tends to favor ENSO growth in all the CGCMs, but at a smaller rate than in observations. In some models it can also promote a phase transition. Longer periods tend to be associated with thermocline and advective feedbacks that are in phase with the SST anomalies, while advective tendencies that lead the SST anomalies by a quarter cycle favor ENSO transitions, thus leading to a shorter period.  相似文献   

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