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1.
冬季北太平洋流场异常主要模态与PDO及NPGO的关系 总被引：1，自引：0，他引：1
采用复经验正交函数(EOF)分解和小波分析,对冬季北太平洋上层海流异常进行了统计动力诊断,并讨论了主要模态与北太平洋年代际振荡(PDO)模态和北太平洋环流振荡(NPGO)模态的关系。结果显示,冬季北太平洋上层洋流异常复EOF分解的第一模态是PDO在流场异常上的反映,第二模态则包含了NPGO的明显信息。主要依据有:(1)第一和第二模态的实时间系数序列分别有准20a和准13a的年代际变化周期,与PDO和NPGO模态的年代际变化周期相同;(2)第一和第二模态实时间系数与北太平洋海表面温度异常(SSTA)的回归系数场的空间分布分别与PDO和NPGO模态的空间结构相近。根据第一和第二模态上层洋流异常计算得到的垂直运动异常的分布,与SSTA的PDO和NPGO模态的空间分布类似,表明海盆尺度流场异常造成的垂直运动是形成PDO和NPGO模态的重要原因。 相似文献
2.
利用第六次国际耦合模式比较计划（Coupled Model Intercomparison Project Phase 6, CMIP6）中的两组子试验,结合线性斜压模式模拟的结果,研究了近年来亚洲内部出现的东亚减少、南亚增加的偶极子型人为气溶胶排放变化调控亚洲夏季风响应的特征及物理机制。对东亚夏季风而言,在考虑海洋-大气耦合作用的气候系统总响应中,东亚夏季风环流和降水显著地加强;在不考虑海洋调控作用的大气直接响应过程中,东亚人为气溶胶排放减少导致的陆地升温使得海陆温差增大,进而通过引起东亚陆地上的气旋式环流异常加强东亚夏季风环流和降水。对南亚夏季风而言,其在偶极子型人为气溶胶强迫下呈现出更为复杂的变化特征。在大气直接响应过程中,人为气溶胶强迫引起的海陆热力差异变化导致南亚夏季风环流减弱、降水减少。在考虑海洋-大气耦合过程的总响应中,南亚夏季风环流表现出微弱增强,同时印度次大陆的南亚夏季风降水也出现增多的异常变化。这表明,局地和海洋-大气动力耦合过程在区域气候对人为气溶胶强迫的响应中扮演着非常重要的角色。此外,通过线性斜压模式发现,东亚和南亚局地的人为气溶胶强迫导致的大气加热场异常不仅能影响局地的夏季风环流,还可以通过引起大范围的表面气压异常进而调控整个亚洲夏季风环流的变化。 相似文献
3.
运用动力学分析的方法，对正压准地转模式中局地热源强迫可能对大气和海洋流场产生的响应结果进行了研究，发现热源扰动和响应流场之间有很好的对应关系，两者具有类似的分布模态，而且“狭窄”的热源扰动可能导致“宽广”的流场响应，这与中低纬大气试验和观测资料的研究结果相符，同时也可部分地解释地球流体中局地热源异常可能导致的环流异常现象。 相似文献
4.
白令海和鄂霍次克海的海冰偶极子及其对大气环流的影响 总被引：3，自引：0，他引：3
基于海冰历史资料的分析表明,白令海和鄂霍次克海的海冰密集度分布在某些年份表现出反位相变化的特征,尤其以冬季最为明显.合成分析的结果表明这种偶极子型海冰异常可能对大气环流(气温和位势高度)产生一定的影响.利用大气环流模式,在给定理想化的白令海、鄂霍次克海偶极子型海冰异常的情况下,通过20个冬季(1-2月)大气环流模式的集合强迫试验,研究了大气环流对这种偶极子型海冰异常的响应特征,数值试验结果与基于观测资料的合成分析比较一致:低空气温对于偶极子型海冰强迫表现为比较明显的对称性响应,气温变化具有垂直斜压的结构,气温变化主要集中在低空;高空大气温度和各层的位势高度的变化均具有显著的非对称性特征,位势高度的变化具有垂直正压结构.参考已有的理论和模拟研究结果,指出高纬地区低空大气的温度变化受直接热力学调整过程的影响明显,对称性响应分量明显,而高层大气温度和各层的大气位势高度变化是由直接热力学调整和间接动力过程响应所共同控制,非对称分量占主导. 相似文献
5.
利用SODA海洋同化资料和NCEP再分析大气资料,分析了热带太平洋次表层海温异常(subsurfaceoceantemperatureanomaly,SOTA)与厄尔尼诺与南方涛动(ElNi?o-SouthernOscillation,ENSO)循环的联系,及SOTA对大气环流的影响。回顾传统ENSO研究,指出存在的问题,提出了ENSO影响大气研究的新思路,得到以下结果:(1)以SOTA为基本资料的研究发现, ENSO事件有两个模态,主要出现在冬季的第一模态对冬季及夏季亚洲-北太平洋-北美地区上空中高纬大气环流有重要影响,主要出现在夏季的第二模态对该地区上空夏季热带和副热带大气系统有重要作用。(2)ENSO事件通过与ENSO相联系的热带太平洋海面温度异常(ENSO-relatedseasurface temperatureanomaly,RSSTA)对大气的异常热通量输送,强迫Walker环流和Hadley环流变化,导致热带和北太平洋及周边地区上空大气环流异常,进而影响相关地区冬季和夏季的气候。(3)海表面温度异常(seasurfacetemperatureanomaly,SSTA)包含RSSTA和大气异常导致的海温变化(sea temperature anomaly caused by atmospheric anomaly, STA)两部分, RSSTA是ENSO事件过程中海洋内部热动力结构调整导致的海面温度变化,在海洋对大气的热输送过程中,它随ENSO事件演变不断更新;STA是大气受RSSTA海洋异常加热后导致的大气环流异常对海面温度的影响,在海洋浅表层STA对RSSTA有重大影响。本文最后讨论了ENSO事件期间热带海洋对大气热输送过程,指出ENSO事件通过海洋内部热动力结构调整产生RSSTA,它直接对大气异常加热,导致大气环流和气候异常,局地海气之间负反馈过程产生STA,反过来抑制RSSTA。结果还指出,人们常用的SSTA变率实际上主要由秋冬季节RSSTA主导,丢失了春夏季ENSO信息,用SSTA研究ENSO事件存在局限性,这也可能是ENSO事件春季预报障碍的原因之一。 相似文献
6.
热带太平洋海洋-大气耦合系统对全球变暖的响应是气候变化的热点问题。前人研究发现,气候模式的模拟偏差对于全球变暖响应结果有重要影响。本文利用美国大气研究中心(National Center for Atmospheric Research, NCAR)的地球系统模式(The Community Earth System Model,CESM)中的大气模式(Community Atmosphere Model version 5, CAM5)设计数值试验,在相同的SST(Sea Surface Temperature)增暖强迫下,通过改变海洋SST的年际变化振幅,来分析热带海洋年际变化强度的模拟对未来热带海区降水和大气环流场未来变化的影响。试验结果表明,随着SST年际变化强度的增加,全球变暖后热带太平洋降水变化的东西不对称性,以及向暖池区域辐合的风场变化等特征都逐渐减弱。进一步的分析发现,不同年际变化信号导致的大气场变化差异主要发生在冬季,是由于热带太平洋SST年际变化主模态ENSO(El Niňo-Southern Oscillation)的不对称性造成的:在厄尔尼诺年,强(弱)的年际变化信号会造成降水在东太平洋产生较大(小)的变化;而在拉尼娜年和正常年份,年际变化信号的强弱对热带降水变化的影响则不大。当热带海温的年际变化较大时,厄尔尼诺年的海温异常更强,造成的降水和风场的变化特征也会更加显著。 相似文献
7.
一个简单的印-太海气耦合模式 总被引：1，自引：0，他引：1
本文基于一层半海洋模式和SVD(Singular Value Decomposition)大气模式构建了一个简单的海气耦合模式, 引入热通量的作用, 分析ENSO影响热带印度洋地区的动力学和热力学耦合过程。其中, 使用统计大气模式, 由给定的SST(Sea Surface Temperature)异常得到风应力异常, 进而驱动海洋环流反馈给SST, 完成海气的动力耦合; 使用块体经验公式由SST异常和风场异常计算热通量异常, 直接作用于SST, 实现海气的热力学耦合。动力耦合实验揭示, 太平洋第一EOF(Empirical Orthogonal Functions) 模态与观测基本吻合。并且模拟Ni?o 3指数存在两年左右的谱峰周期。这说明, 海气动力学耦合是ENSO生成的主要因素。热力耦合的加入是为了考察ENSO影响热带印度洋的热力学效应。同时考虑动力和热力耦合的实验结果表明, 热带太平洋暖异常中心更加接近观测值, 热带印度洋出现海盆尺度海温正异常。这意味着热带太平洋的ENSO信号通过海气界面的热量交换实现对热带印度洋地区的遥强迫, 导致印度洋海盆尺度增暖。 相似文献
8.
中等海气耦合模式对外强迫响应试验方案的能力检验 总被引：1，自引：1，他引：0
针对如何得到海洋-大气耦合模式对某外强迫场响应的问题,提出了2种数值试验方案:外加方案和替代方案,并对上述2个方案利用中等海洋-大气耦合模式进行了检验.检验结果表明,运用2个方案中的任何一个都可以基本上达到用该模式模拟对强迫场响应的目的;用海面风强迫的外加方案得到响应场的变化在位相准确性上较好,但会夸大响应场的振幅;在替代方案中,模式对海面风强迫的响应要比对海温强迫的响应更准确. 相似文献
9.
全球海洋环流模式中上层海洋对表面强迫的响应和调整 I. 年际变率 总被引：1，自引：1，他引：1
利用一个较高分辨率的全球海洋环流模式在COADS1945～1993年逐月平均资料的强迫下对海温和环流场进行了模拟试验,研究了全球热带海洋(主要是热带太平洋)海温和环流场的年际变化特征及模式ENSO冷暖事件演变的控制机理.结果表明,模式成功地再现了和观测一致的海温和环流的年际变化以及ENSO演变特征.其中热带印度洋年际SST变率的主要模态表现为与ENSO相联系的海盆尺度的一致性增暖或变冷现象,次级模态为热带印度洋偶极子模态;热带大西洋的SST年际变率表现为类ENSO的年际振荡现象.在热带太平洋,SST年际变化主要表现为ENSO型,环流的年际变率表现为与ENSO相对应的热带海洋质量循环圈的年际异常.对应于暖(冷)事件,前期赤道海洋垂直环流圈显示出减弱(增强)的特征.其中南赤道流异常的位相较Nino3区海温总体要超前5个月左右的时间;赤道上翻流异常的位相在表层要超前4个月,并随时间由上至下扩展;赤道潜流的异常则显示出东传特征,其中最早的较为显著的异常发生ENSO成熟前3个月180°附近.在模式ENSO冷暖事件的演变过程中,次表层海温异常沿赤道的东传起了关键作用,模式的ENSO模态主要表现为"时滞振子"模态. 相似文献
10.
全球海洋环流模式中上层海洋对表面强迫的响应和调整Ⅰ.年际变率 总被引：1，自引：1，他引：0
利用一个较高分辨率的全球海洋环流模式在COADS 1945～1993年逐月平均资料的强迫下对海温和环流场进行了模拟试验,研究了全球热带海洋(主要是热带太平洋)海温和环流场的年际变化特征及模式ENSO冷暖事件演变的控制机理.结果表明,模式成功地再现了和观测一致的海温和环流的年际变化以及ENSO演变特征.其中热带印度洋年际SST变率的主要模态表现为与ENSO相联系的海盆尺度的一致性增暖或变冷现象,次级模态为热带印度洋偶极子模态;热带大西洋的SST年际变率表现为类ENSO的年际振荡现象.在热带太平洋,SST年际变化主要表现为ENSO型,环流的年际变率表现为与ENSO相对应的热带海洋质量循环圈的年际异常.对应于暖(冷)事件,前期赤道海洋垂直环流圈显示出减弱(增强)的特征.其中南赤道流异常的位相较Nino3区海温总体要超前5个月左右的时间;赤道上翻流异常的位相在表层要超前4个月,并随时间由上至下扩展;赤道潜流的异常则显示出东传特征,其中最早的较为显著的异常发生ENSO成熟前3个月180°附近.在模式ENSO冷暖事件的演变过程中,次表层海温异常沿赤道的东传起了关键作用,模式的ENSO模态主要表现为"时滞振子"模态. 相似文献
11.
A process-oriented, quasi-geostrophic, barotropic model has been developed with the aim of studying the relative importance of wind and topographic forcing on oceanic eddy generation by tall, deep water islands. As a case study, we chose the island of Gran Canaria. Topographic forcing was established using different intensities (weak, medium, strong, and very strong) for the oceanic current incident to the island. Wind forcing was introduced to simulate the mean wind curl observed in atmospheric tall island wakes. As observed from in situ data, the resulting wind curl consists of two cells of opposite sign which become a complementary source of vorticity at the island lee. The intensity and the shape of the two cells depend on the strength of the incident wind against the obstacle. The oceanic model was forced at three different wind (trade winds) speeds which correspond to weak, medium and strong wind intensities. Results from several numerical experiments show that in those periods where the incident wind is in the medium–strong range and the incident current speed is low (low Reynolds number), the wind forcing is the trigger mechanism for oceanic eddy generation. Eddies are spun off from the island for a lower Reynolds number (Re)/intensity of the oceanic flow (Re = 20) when compared with only topographic forcing (Re > 60). However, when the current speed is strong (high Reynolds number), the vorticity input by the wind is quickly advected by the oceanic flow and does not contribute to oceanic eddy generation. When only wind forcing is considered, only two stationary eddies are generated in the island wake. In this case, eddies of opposite sign are not sequentially spun off by the island and a Von-Kármán-like eddy street is not developed downstream of the island. Therefore, the main mechanism responsible for the development of an eddy street is the topographic perturbation of the oceanic flow by the island flanks. The wind over the island wake acts only as an additional source of vorticity, promoting the generation of an eddy street at a lower intensity of the incident oceanic flow, but not being capable of generating an eddy street without the topographic forcing. 相似文献
12.
The homogeneous residual circulation in Hauraki Gulf arising from the tides, steady winds, and oceanic inflows is considered by use of a depth‐averaged 2‐dimensional numerical model. Vertical current structure of the wind‐driven circulation is derived by using the computed wind‐induced sea surface slopes, the wind stress, and a prescribed vertical eddy viscosity. Tidal residual circulation is weak, less than 0.01 ms‐1 over most of the Gulf. The response of the Gulf to wind‐forcing indicates a preference for north‐west/south‐east directed winds, the flow through the Gulf being more than 3 times as strong as for winds from other directions. Surface currents are mainly in the wind direction, but subsurface currents reveal closed circulation cells in near‐coastal areas. Simple oceanic inflows give rise to water movements which penetrate to the inner part of the Gulf. 相似文献
13.
利用一个两层半的热带海洋模式,采用数值实验的方法研究了热带海洋对于初始海洋混合层深度异常和大气季节内时间尺度热力强迫激发产生的Ｒｏｓｓｂｙ波和Ｋｅｌｖｉｎ波。研究表明,初始海洋混合层深度异常和大气热力强迫,可以在两层半热带海洋模式中激发产生东向传播具有Ｋｅｌｖｉｎ波性质的波动和具有Ｒｏｓｓｂｙ波性质的波动。热力强迫激发产生海洋Ｒｏｓｓｂｙ波和Ｋｅｌｖｉｎ波所需时间长于初始海洋混合层深度异常和大气季节内动力强迫激发产生两波所需时间,与大气季节内动力强迫激发的Ｒｏｓｓｂｙ波相比,初始深度异常与大气热力强迫激发产生Ｒｏｓｓｂｙ波具有不同的热力性质。 相似文献
14.
C. Langlais B. Barnier J.M. Molines P. Frauni D. Jacob S. Kotlarski 《Ocean Modelling》2009,30(4):270-286
The paper evaluates atmospheric reanalysis as possible forcing of model simulations of the ocean circulation inter-annual variability in the Gulf of Lions in the Western Mediterranean Sea between 1990 and 2000. The sensitivity of the coastal atmospheric patterns to the model resolution is investigated using the REMO regional climate model (18 km, 1 h), and the recent global atmospheric reanalysis ERA40 (125 km, 6 h). At scales from a few years to a few days, both atmospheric data sets exhibit a very similar weather, and agreement between REMO and ERA40 is especially good on the seasonal cycle and at the daily variability scale. At smaller scales, REMO reproduces more realistic spatio-temporal patterns in the ocean forcing: specific wind systems, particular atmospheric behaviour on the shelf, diurnal cycle, sea-breeze. Ocean twin experiments (1990–1993) clearly underline REMO skills to drive dominant oceanic processes in this microtidal area. Finer wind patterns induce a more realistic circulation and hydrology of the shelf water: unique shelf circulation, upwelling, temperature and salinity exchanges at the shelf break. The hourly sampling of REMO introduces a diurnal forcing which enhances the behaviour of the ocean mixed layer. In addition, the more numerous wind extremes modify the exchanges at the shelf break: favouring the export of dense shelf water, enhancing the mesoscale variability and the interactions of the along slope current with the bathymetry. 相似文献
15.
The present study documents the atmosphere–ocean interaction in interannual variations over the South China Sea (SCS). The atmosphere–ocean relationship displays remarkable seasonality and regionality, with an atmospheric forcing dominant in the northern and central SCS during the local warm season, and an oceanic forcing in the northern SCS during the local cold season. During April–June, the atmospheric impact on the sea surface temperature (SST) change is characterized by a prominent cloud-radiation effect in the central SCS, a wind-evaporation effect in the central and southern SCS, and a wind-driven oceanic effect along the west coast. During November–January, regional convection responds to the SST forcing in the northern SCS through modulation of the low-level convergence and atmospheric stability. Evaluation of the precipitation–SST and precipitation–SST tendency correlation in 24 selected models from CMIP5 indicates that the simulated atmosphere–ocean relationship varies widely among the models. Most models have the worst performance in spring. On average, the models simulate better the atmospheric forcing than the oceanic forcing. Improvements are needed for many models before they can be used to understand the regional atmosphere–ocean interactions in the SCS region. 相似文献
16.
《Ocean Modelling》2008,20(3):240-251
Using new global satellite remote sensing data, we show that ignoring the ocean current dependence in the wind stress artificially increases global wind power input to the oceanic general circulation by about 32%, and more than doubles the input in the regions of strong ocean current systems. Scatterometer-derived wind stress naturally accounts for the moving ocean that is not included in traditional wind stress products. However, forcing an ocean model with a scatterometer-derived wind stress cannot actually account for the ocean current effect on the wind power input. The difference between the real and modeled surface eddy fields can reduce the damping associated with the ocean current dependence in wind stress, leading to a positive bias in global wind power input of about 23%. Most of this spurious energy flux goes directly to the fluctuation eddy field and is several times larger than the energy flux to real ocean eddies. 相似文献
17.
The formation of the South China Sea (SCS) deep basin warm-core and cool-core eddies was studied numerically using the Princeton
Ocean Model (POM) with 20 km horizontal resolution and 23 sigma levels conforming to a realistic bottom topography. Numerical
integration was divided into pre-experimental and experimental stages. During the pre-experimental stage, we integrated the
POM model for three years from zero velocity and April temperature and salinity climatological fields with climatological
monthly mean wind stresses, restoring type surface salt and heat fluxes, and observational oceanic inflow/outflow at the open
boundaries. During the experimental stage, we integrated the POM model for another 16 months under three different conditions:
one control and two sensitivity runs (no-wind and no lateral transport). We take the fields of the last 12 months for analysis.
The simulation under control run agrees well with earlier observational studies on the South China Sea surface thermal variabilities.
In addition, the sensitivity study further confirms that the wind effect is the key factor for generation of the SCS deep
basin warm/cool eddy and that the lateral boundary forcing is the major factor for the formation of the strong western boundary
currents, especially along the southeast Chinese coast during both summer and winter monsoon seasons. 相似文献
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For more and more applications in coastal and offshore engineering, numerical simulations of waves and surges are required. An important input parameter for such simulations are wind fields. They represent one of the major sources for uncertainties in wave and surge simulations. Wind fields for such simulations are frequently obtained from numerical hindcasts with regional atmospheric models (RAMs). The skill of these atmospheric hindcasts depends, among others, on the quality of the forcing at the boundaries. Furthermore, results may vary due to uncertainties in the initial conditions. By comparing different existing approaches for forcing a regional atmospheric model, it is shown that the models' sensitivity to uncertainties in the initial conditions may be reduced when a more sophisticated approach is used that has been suggested recently. For a specific, although somewhat brief test period, it is demonstrated that an improved hindcast skill for near surface wind fields is obtained when this approach is adopted. Consequences of the reduced uncertainty in wield fields for the hindcast skill of subsequent wave modelling studies are demonstrated. Recently, this new approach has been used together with a regional atmosphere model to produce a 40-year wind hindcast for the Northeast Atlantic, the North Sea and the Baltic Sea. The hindcast is presently extended to other areas and the wind fields are used to produce 40-year high-resolution hindcasts of waves and surges for various European coastal areas. 相似文献
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风应力桥梁作用下热带太平洋和热带印度洋相互作用的数值试验 总被引：1，自引：1，他引：0
利用中等复杂程度全球热带大气和热带海洋模式的数值试验,模拟分析了热带太平洋和热带印度洋通过风应力桥梁的相互作用过程.利用NCEP再分析的1958～1998年SST强迫大气模式得到的风应力与NCEP再分析的同期热通量共同驱动海洋模式,作为控制试验;和控制试验平行,但强迫大气模式的SST在某一海盆取为多年气候平均值的试验作为敏感性试验.比较控制试验与敏感性试验模拟的SST变率,揭示了热带某海盆SST异常通过风应力桥梁作用对其他海盆SST的影响及其过程.数值试验结果表明:热带某海盆SST暖(冷)异常一般总是引起该海盆上空西部西(东)风异常和东部东(西)风异常;热带太平洋SST暖(冷)异常导致年际尺度上印度洋上空东(西)风异常和年代际尺度上热带印度洋风场辐散(合),该风应力导致热带印度洋年际SST暖(冷)异常以及年代际SST冷(暖)异常,但这种异常均较弱;热带印度洋SST暖(冷)异常导致热带太平洋上空东(西)风异常,该风应力异常在年际和年代际尺度上均导致热带太平洋SST冷(暖)异常,但年代际尺度上异常更明显.考虑到热带印度洋SSTA受热带太平洋SSTA影响大,并且热带太平洋SST暖(冷)异常主要通过表面热通量导致热带印度洋SST变暖(冷)的观测事实,文中揭示的热带印度洋SST暖(冷)异常通过风应力桥梁作用导致热带太平洋SST冷(暖)异常的结果表明,热带印度洋SSTA对于热带太平洋SSTA主要起着一种负反馈作用,并且这种负反馈作用在年代际尺度上更为明显. 相似文献