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1.
西太平洋副热带高压的年际变率受热带多个关键海区的海-气相互作用过程调控, 但彼此间的因果关联和影响机制尚不清楚。为揭示西太平洋副热带高压的年际变率与热带海温及大气环流异常之间的内在关联特性, 定义了三个关键海区以及赤道纬向西风区的特征指数, 并分别与西太平洋副热带高压强度、脊线指数进行了交叉小波和相干小波分析。研究发现:西太平洋副热带高压指数存在显著的2~3年和准5年的周期振荡, 20世纪八九十年代后, 由于暖池区海温及赤道纬向西风区的Hadley环流强迫加强, 致使副热带高压特征指数的2~3年周期振荡加强; 从位相关系看, 先是西太平洋副热带高压减弱南撤导致纬向西风加强, 其后影响赤道东太平洋海温升高, 同时暖水向东传, 使赤道中太平洋以及暖池区海温逐渐升高, 在Hadley环流作用下使副高加强北抬。基于上述西太平洋副热带高压的年际变率与热带海温及大气环流异常变化相关性诊断研究, 进一步探讨了造成这种相关性的影响机理和因果关联, 为揭示西太平洋副热带高压年际变率与热带海温及大气环流异常的相关性做探索研究。   相似文献   

2.
选取1952-2005年北太平洋月平均海表温度(SST)资料,经过奇异值分解分析表明:6月份日界线附近西风漂流区的海温集中了北太平洋海温场的主要信息,西风漂流区与赤道冷水区的海温存在遥相关震荡,并且在6月份达到全年的最高值,11月份其振幅出现次高值。6月西风漂流区的海温(SST)可视为来年盛夏(7-8月)西太平洋副热带高压的强弱变化的信号:当6月份西风漂流区的海温(SST)偏低,则来年盛夏西太平洋副热带高压偏强;反之,则来年盛夏西太平洋副热带高压偏弱。  相似文献   

3.
北太平洋海平面气压场变化与海温的关系   总被引:1,自引:0,他引:1  
利用SVD(singular value decomposition)方法分析了1948年1月—2002年12月北太平洋海平面气压场与海温的关系。结果表明,SVD第1对异类相关分布型反映出,当东北太平洋副热带高压加强(减弱)时,Namias海区海温升高(降低),而加利福尼亚海流区海温降低(升高)。SVD第2对异类相关分布型表明,当阿留申低压加深、北太平洋副热带地区气压升高时,黑潮暖流区海温升高,而北太平洋高、低纬海温降低;反之亦然。时滞相关表明,北太平洋大气环流异常超前海温1个月的相关最好,海温变化对大气环流异常分布型具有维持作用。NCAR CCSM3模拟结果很好地验证了上述结论,即在海气相互作用过程中,东北太平洋副热带高压和NPO(North Pacific Oscillation)与北太平洋海温存在密切联系。  相似文献   

4.
北太平洋中纬度负海温异常对副热带高压影响的数值试验   总被引:3,自引:2,他引:3  
利用中国科学院大气物理研究所的T42L9全球大气环流模式,研究了1993年夏季北太平洋中纬度海温异常对西太平洋副热带高压的影响。数值试验结果表明:(1)中纬度地区负距平海温异常对其南侧太平洋副热带高压的形态和脊线位置都有影响,负距平海温异常试验的500hPa副热带高压的形态明显比气候平均海温试验更接近于NCEP资料实况,对流层中下层副热带高压脊线的平均位置也比气候平均海温试验要偏南,与实况比也更接近了;(2)在500hPa上,北太平洋中纬度负距平海温异常在其南侧产生的高度扰动使副热带高压向南偏移,而在其北侧产生的高度扰动则沿北太平洋中高纬度、北美中高纬度、北大西洋和欧洲南部以及地中海和北非地区的大圆路径传播,并影响和改变整个北半球大气环流的变化。1993年夏季北太平洋中纬度异常的低海温可能是该年盛夏6、7月北太平洋副热带高压位置异常偏南的重要原因之一。  相似文献   

5.
刘珊  李栋梁 《高原气象》2009,28(4):711-722
利用青海、 西藏59个测站1971-2004年夏季(6~8月)的月平均气温和北太平洋(10°S~50°N、 120°E~80°W)1970-2003年的冬季(上年12月~次年2月)平均海表温度, 通过EOF、 REOF、 SVD等方法, 对青藏高原地区夏季气温和前期冬季北太平洋海温的异常特性以及两者之间的空间遥相关特征进行了研究, 并对北太平洋冬季海温及青藏高原夏季气温的年代际空间特征进行了分析。结果表明, 北太平洋冬季海温的异常分布型有: (1)赤道中东太平洋与西北太平洋海温相反分布型, (2)副热带北太平洋海温东西反相分布型, (3)北太平洋海温南北反相分布型, (4)北太平洋海温东西一致分布型。其中赤道中东太平洋与西北太平洋海温反相变化是冬季北太平洋SSTA的主要空间分布特征。进一步分析表明, 北太平洋冬季海温可分为6个气候区: 赤道中东太平洋区、 加利福尼亚海流区、 黑潮区、 亲潮区、 阿拉斯加海流区和中太平洋区。青藏高原地区夏季气温的异常分布型主要为(1)全区一致的偏高(低)型, (2)南北相反分布型, (3)周边地区与腹地相反分布型。青藏高原夏季气温可分为4个主要气候区: 东北部区、 西藏东南部区、 中部区和南部边缘区。冬季赤道中东太平洋SSTA 与次年夏季青藏高原地区区域性温度异常之间有较为明显的负相关关系, 这种关系在两者的其它空间关系中是第一位的。  相似文献   

6.
太平洋海气相互作用的时空变化   总被引:11,自引:2,他引:11  
陈烈庭 《气象学报》1983,41(3):296-304
本文根据1957—1976年赤道太平洋海温和北太平洋海平面气压的月平均资料,计算了它们之间全年(1—12月)逐月的时滞相关,分析了北太平洋副热带反气旋影响赤道海温和赤道海温对副高反馈的季节变化。发现它们之间的联系不同季节、不同地区有明显差异:副热带反气旋对赤道海温的影响(负相关)以春季最大,秋季最小;赤道海温的反馈,对副高的不同部分作用不同,对副高主体的作用(正相关)以冬半年最大、夏半年较小(尤其是盛夏),对西部副高脊的作用(负相关)相反,以夏半年最大,冬半年较小。其过渡期为5月和11月。同时对其季节变化的可能原因也提出了一些初步看法。其中特别强调了大型环流背景的基本状态(包括平均垂直环流)对海气相互作用过程的重要性。  相似文献   

7.
王永光  郑志海 《气象》2018,44(4):565-571
2017年夏季(2017年6—8月),全国平均降水量348.6 mm,较常年同期(322.6 mm)偏多8.1%,呈现南、北两条多雨带。东亚夏季风偏弱,西太平洋副热带高压显著偏强,脊线位置偏南;欧亚中高纬呈现“两槽一脊”环流型,贝加尔湖地区为正距平控制。赤道中东太平洋海温从前冬冷水向春、夏季暖水发展,20世纪80年代以来容易出现南方多雨的Ⅳ类雨型,夏季贝加尔湖阻塞高压发展。2017年赤道中东太平洋海温从前冬冷水向春、夏季暖水发展,春季北大西洋三极子正位相和2016年欧亚积雪从秋到冬的减少,均有利于夏季贝加尔湖阻塞高压发展,这是夏季主要多雨带位于长江以南的重要前兆信号。  相似文献   

8.
2017年夏季(2017年6—8月),全国平均降水量348.6mm,较常年同期(322.6mm)偏多8.1%,呈现南、北两条多雨带。东亚夏季风偏弱,西太平洋副热带高压显著偏强,脊线位置偏南;欧亚中高纬呈现"两槽一脊"环流型,贝加尔湖地区为正距平控制。赤道中东太平洋海温从前冬冷水向春、夏季暖水发展,20世纪80年代以来容易出现南方多雨的Ⅳ类雨型,夏季贝加尔湖阻塞高压发展。2017年赤道中东太平洋海温从前冬冷水向春、夏季暖水发展,春季北大西洋三极子正位相和2016年欧亚积雪从秋到冬的减少,均有利于夏季贝加尔湖阻塞高压发展,这是夏季主要多雨带位于长江以南的重要前兆信号。  相似文献   

9.
厄尼诺现象与北半球500百帕大气环流   总被引:1,自引:0,他引:1       下载免费PDF全文
本文计算了赤道东太平洋海面温度与北半球500百帕大气环流的遥相关,发现它们之间的遥相关现象是十分显著的。从相关场的空间分布看,赤道东太平洋海面温度与热带低纬度地区500百帕高度全年为较强的正相关,而与中高纬度地区500百帕高度有较强的负相关。相关最好的地区,低纬度主要在太平洋西部,向西至南海、印度洋、阿拉伯海,其次在大西洋上。中高纬度的太平洋中部和北部,以及北美中部至大西洋上为较强的负相关。在欧亚大陆西部,通过北极区至北美大陆西北部则有稍弱的正相关。通过这一正相关区中心,似乎存在着一个对称轴,使得太平洋及欧亚地区的相关场与北美和大西洋地区的相关场呈轴对称,此对称轴随季节的差异在极地附近有东西半球之间的摆动。同时发现,从热带太平洋—欧亚大陆东部,北太平洋中部和北部—北极—北美大陆东部,北大西洋北部—热带大西洋西部,存在着一种相关区正、负间隔的“大圆环路”。从时间上看,赤道东太平洋海面温度的变化对北半球500百帕大气环流的影响是持续的,一般海温超前的影响很明显,往往超前达一年之久,较强的影响超前约5、6个月左右。海温滞后的相关与超前的相关符号相反。厄尼诺现象对北半球冬季极涡、西风带槽脊、副热带急流以及副热带高压都有影响,尤其是对西太平洋副热带高压,以及我国长江流域梅雨的影响更为明显。  相似文献   

10.
长江下游夏季降水与东亚夏季风及春季太平洋海温的关系   总被引:12,自引:5,他引:7  
利用NCEP/NCAR逐日再分析资料、NOAA月平均海表温度资料及中国站点逐日降水资料,研究了长江下游夏季降水、东亚夏季风(区分南海热带夏季风和副热带夏季风)及春季太平洋海温之间的关系。结果表明,南海夏季风强度与长江下游夏季降水量呈反相关,而副热带夏季风强度与长江下游夏季降水量呈正相关;春季赤道东太平洋海温与当年长江下游夏季降水存在正相关,是夏季长江下游夏季降水变化趋势的较好前期预测信号;南海夏季风和副热带夏季风强度对春季赤道东太平洋海温异常的响应是相反的。  相似文献   

11.
In this study, dynamic linkage of atmosphere-ocean coupling between the North Pacific and the tropical Pacific was demonstrated using a large number of ensemble perturbed initial condition experiments in a fully coupled fast ocean-atmosphere model (FOAM). In the FOAM model, an idealized mixed layer warming was initiated in the Kuroshio-Oyashio extension region, while the ocean and atmosphere remained fully coupled both locally and elsewhere. The modeling results show that the warm anomalies are associated with anomalous cyclonic winds, which induce initial warming anomalies extending downstream in the following winter. Then, the downstream warming spreads southwestward and induces SST warming in the equatorial Pacific via surface wind-evaporation-SST feedback. Warming in the tropical Pacific is further reinforced by Bjerknes’ feedback.  相似文献   

12.
The North Pacific Oscillation (NPO) recently (re-)emerged in the literature as a key atmospheric mode in Northern Hemisphere climate variability, especially in the Pacific sector. Defined as a dipole of sea level pressure (SLP) between, roughly, Alaska and Hawaii, the NPO is connected with downstream weather conditions over North America, serves as the atmospheric forcing pattern of the North Pacific Gyre Oscillation (NPGO), and is a potential mechanism linking extratropical atmospheric variability to El Ni?o events in the tropical Pacific. This paper explores further the forcing dynamics of the NPO and, in particular, that of its individual poles. Using observational data and experiments with a simple atmospheric general circulation model (AGCM), we illustrate that the southern pole of the NPO (i.e., the one near Hawaii) contains significant power at low frequencies (7–10?years), while the northern pole (i.e., the one near Alaska) has no dominant frequencies. When examining the low-frequency content of the NPO and its poles separately, we discover that low-frequency variations (periods >7?years) of the NPO (particularly its subtropical node) are intimately tied to variability in central equatorial Pacific sea surface temperatures (SSTs) associated with the El Ni?o-Modoki/Central Pacific Warming (CPW) phenomenon. This result suggests that fluctuations in subtropical North Pacific SLP are important to monitor for Pacific low-frequency climate change. Using the simple AGCM, we also illustrate that variability in central tropical Pacific SSTs drives a significant fraction of variability of the southern node of the NPO. Taken together, the results highlight important links between secondary modes (i.e., CPW-NPO-NPGO) in Pacific decadal variability, akin to already established relationships between the primary modes of Pacific climate variability (i.e., canonical El Ni?o, the Aleutian Low, and the Pacific Decadal Oscillation).  相似文献   

13.
Future climate in the Pacific Northwest   总被引:4,自引:2,他引:2  
Climate models used in the Intergovernmental Panel on Climate Change (IPCC) Fourth Assessment Report (AR4) on the whole reproduce the observed seasonal cycle and twentieth century warming trend of 0.8°C (1.5°F) in the Pacific Northwest, and point to much greater warming for the next century. These models project increases in annual temperature of, on average, 1.1°C (2.0°F) by the 2020s, 1.8°C (3.2°F) by the 2040s, and 3.0°C (5.3°F) by the 2080s, compared with the average from 1970 to 1999, averaged across all climate models. Rates of warming range from 0.1°C to 0.6°C (0.2°F to 1.0°F) per decade. Projected changes in annual precipitation, averaged over all models, are small (+1% to +2%), but some models project an enhanced seasonal cycle with changes toward wetter autumns and winters and drier summers. Changes in nearshore sea surface temperatures, though smaller than on land, are likely to substantially exceed interannual variability, but coastal upwelling changes little. Rates of twenty-first century sea level rise will depend on poorly known factors like ice sheet instability in Greenland and Antarctica, and could be as low as twentieth century values (20 cm, 8) or as large as 1.3 m (50).  相似文献   

14.
It is shown that the salinity minimum at subsurface depths of the tropical Pacific is a local phenomenon. Characteristics of the salinity minimum are relative by absolute values and variable in time. It appears and disappears in the intertropical convergence zone according to variability of the freshwater budget sign. The salinity minimum appears during the negative phase of the freshwater budget on the background of the previous freshening of the sea surface. The salinity minimum at intermediate depths in both hemispheres is a single phenomenon of climatic time scale. At present, it exists at intermediate layers in the arid zones of both hemispheres due to the negative phase of the freshwater budget. This minimum is related to the Earth climate system variability at the geological time scale. Differences in its properties in the Northern and Southern hemispheres reflect differences in the freshwater budget values and the duration of their influence at the geological time scale.  相似文献   

15.
Analyzed is the variability of seasonal salinity in the North Pacific. It is demonstrated that the formation and disappearance of salinity minimum in subsurface layers depends on the freshwater budget variability of different time scales. In general, the salinity minimum is a temporary phenomenon formed during the negative phase of freshwater budget, when the evaporation exceeds the precipitation. Seasonal variability of fresh water budget leads to the seasonal formation of salinity minimum on the boundary between the climatic zones. The existence of salinity minimum at intermediate depths in the tropics is caused by the negative phase of long-period variability of freshwater budget.  相似文献   

16.
Procedures have been implemented at the Climate Analysis Center of the National Meteorological Center (CAC/NMC) to provide montly hindcasts of oceanographic conditions in the tropical Pacific. A central component of this system is a primitive equation ocean general circulation model that was developed at the Geophysical Fluid Dynamics Laboratory (GFDL). This is forced with monthly mean fields for wind stress and net heat flux. Until recently the former were derived from ship reports available on the Global Telecommunication System (GTS). The heat fluxes are slightly modified climatological fluxes from Esbensen and Kushnir. To correct for errors in the simulations, thermal data in the upper 450 and surface-temperature data are assimilated montly.Numerical experiments were run to examine the sensitivity of the simulations to small changes in the stress fields. Variations of the drag coefficient by 15% result in differences in sea-surface temperature (SST) and subsurface thermal structure in the eastern Pacific that are comparable with the observed annual and interannual variability. Comparisons with simulations in which the wind stresses were derived from operational atmospheric analyses show sensitivities of the same magnitude. Comparisons of simulations forced either with these of ship-recorded winds to a run with data assimilation show that significant errors are found in both, especially in the off-equatorial regions. Consequently, until forcing fields are improved, accurate simulations will require the use of data assimilation.  相似文献   

17.
Decadal atmosphere-ocean variations in the Pacific   总被引:67,自引:7,他引:60  
Considerable evidence has emerged of a substantial decade-long change in the north Pacific atmosphere and ocean lasting from about 1976 to 1988. Observed significant changes in the atmospheric circulation throughout the troposphere revealed a deeper and eastward shifted Aleutian low pressure system in the winter half year which advected warmer and moister air along the west coast of North America and into Alaska and colder air over the north Pacific. Consequently, there were increases in temperatures and sea surface temperatures (SSTs) along the west coast of North America and Alaska but decreases in SSTs over the central north Pacific, as well as changes in coastal rainfall and streamflow, and decreases in sea ice in the Bering Sea. Associated changes occurred in the surface wind stress, and, by inference, in the Sverdrup transport in the north Pacific Ocean. Changes in the monthly mean flow were accompanied by a southward shift in the storm tracks and associated synoptic eddy activity and in the surface ocean sensible and latent heat fluxes. In addition to the changes in the physical environment, the deeper Aleutian low increased the nutrient supply as seen through increases in total chlorophyll in the water column, phytoplankton and zooplankton. These changes, along with the altered ocean currents and temperatures, changed the migration patterns and increased the stock of many fish species. A north Pacific (NP) index is defined to measure the decadal variations, and the temporal variability of the index is explored on daily, annual, interannual and decadal time scales. The dominant atmosphere-ocean relation in the north Pacific is one where atmospheric changes lead SSTs by one to two months. However, strong ties are revealed with events in the tropical Pacific, with changes in tropical Pacific SSTs leading SSTs in the north Pacific by three months. Changes in the storm tracks in the north Pacific help to reinforce and maintain the anomalous circulation in the upper troposphere. A hypothesis is put forward outlining the tropical and extratropical realtionships which stresses the role of tropical forcing but with important feed-backs in the extratropics that serve to emphasize the decadal relative to interannual time scales. The Pacific decadal timescale variations are linked to recent changes in the frequency and intensity of El Niño versus La Nina events but whether climate change associated with global warming is a factor is an open question.The National Center for Atmospheric Research is sponsored by the National Science Foundation  相似文献   

18.
In this study, we investigate the impact of atmospheric convection over the western tropical Pacific (100–145°E, 0–20°N) on the boreal winter North Pacific atmosphere flow by analyzing National Center for Environmental Prediction Reanalysis 1, Extended Reconstructed Sea Surface Temperature and Global Precipitation Climatology Project data. The western tropical Pacific convection is not only the main energy source driving the local Hadley and Walker circulations, but it also significantly influences North Pacific circulation, by modifying a mid-latitude Jet stream through the connection with the local Hadley circulation. On the one hand, this strong convection leads to a northward expansion of local Hadley cells simultaneous with a northward movement of the western North Pacific jet because of the close correlation between the Jet and Hadley circulation boundaries. On the other hand, this strong convection also intensifies tropical Pacific Walker circulation, which reduces the eastern Pacific sea surface temperature, resembling a La Nina state through the enhanced equatorial upwelling. The cooling of the eastern tropical Pacific has an inter-tropical convergence zone located further north; thus, the local Hadley circulation moves northward. As a result, the jet axis over the eastern North Pacific, which also corresponds to the boundary of the local Hadley circulation, moves to higher latitude. Consequently, this northward movement of the Jet axis over the North Pacific is reflected as a northwest–southeast dipole sea level pressure (SLP) pattern. The composite analysis of SLP over the North Pacific against the omega (Ω) (Pa/s) at 500 hPa over the western tropical Pacific actually reveals that this northwest-southeast dipole structure is attributed to the intensified tropical western Pacific convection, which pushes the Pacific Jet to the north. Finally we also analyzed south Pacific for the austral winter as did previously to North Pacific, and found that the results were consistent.  相似文献   

19.
The present study examines the relationship between two types of El Niño–Southern Oscillation (ENSO), the central Pacific (CP) ENSO and the eastern Pacific (EP) ENSO, and the sea surface temperature (SST) variability over the South Pacific (SP) (20° S–60° S, 145° E–70° W) using NOAA OI SST for the period 1982–2006. The SP SST variability associated with the two types of ENSO varies with season. These two types of ENSO can excite different atmospheric patterns associated with the Pacific–South American mode, through which they influence the SP SST variability. Both the surface turbulent air–sea heat fluxes and the heat advection by Ekman currents (i.e., Ekman heat fluxes) have an important impact on the SST variability. An analysis of the surface mixed layer heat budget indicates that the heat fluxes (the sum of turbulent heat fluxes and Ekman heat fluxes) can effectively explain much of the SST variability related to the two types of ENSO.  相似文献   

20.
Based on observational and reanalysis data,the relationships between the eastern Pacific(EP)and central Pacific(CP)types of El Ni?o?Southern Oscillation(ENSO)during the developing summer and the South Asian summer monsoon(SASM)are examined.The roles of these two types of ENSO on the SASM experienced notable multidecadal modulation in the late 1970s.While the inverse relationship between the EP type of ENSO and the SASM has weakened dramatically,the CP type of ENSO plays a far more prominent role in producing anomalous Indian monsoon rainfall after the late 1970s.The drought-producing El Ni?o warming of both the EP and CP types can excite anomalous rising motion of the Walker circulation concentrated in the equatorial central Pacific around 160°W to the date line.Accordingly,compensatory subsidence anomalies are evident from the Maritime Continent to the Indian subcontinent,leading to suppressed convection and decreased precipitation over these regions.Moreover,anomalously less moisture flux into South Asia associated with developing EP El Ni?o and significant northwesterly anomalies dominating over southern India accompanied by developing CP El Ni?o,may also have been responsible for the Indian monsoon droughts during the pre-1979 and post-1979 sub-periods,respectively.El Ni?o events with the same“flavor”may not necessarily produce consistent Indian monsoon rainfall anomalies,while similar Indian monsoon droughts may be induced by different types of El Ni?o,implying high sensitivity of monsoonal precipitation to the detailed configuration of ENSO forcing imposed on the tropical Pacific.  相似文献   

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