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1.
北极涡年代际变化及其与我国春季降水的关系 总被引：8，自引：0，他引：8
基于NCEP/NCAR的500hPa再分析高度场资料计算出多年北半球及各分区的极涡面积和强度,利用线性倾向估计、小波分析及二项式滑动平均分析极涡及我国春季降水的年代际变化特征,并采用奇异值分解讨论同期及前期极涡对我国春季降水的影响。各季节极涡面积及强度均存在显著的年代际变化,在20世纪70年代中期之前有上升趋势,而后出现下降的趋势;但极涡面积总体上有显著的线性变小趋势。在60年代中前期极涡位置偏向亚欧大陆,在90年代中后期极涡位置有偏向太平洋和大西洋一带趋势。我国160站平均春季降水量经历较明显的3次上升过程和4次下降过程;华南、西南地区春季降水趋势与长江流域、黄河流域呈现两种相反的分布型;在20世纪60年代中前期、90年代初及末期,长江流域、黄河流域春季降水量偏多,而在80年代末期、90年代中期及本世纪初,华南、西南地区出现偏多。在春季,若II区(150°E～120°W)极涡面积异常大,I区(60～150°E)、III区(120～30°W)极涡强度异常弱,长江、黄河之间中游地区的降水出现负距平,广东、福建沿海降水出现正距平。前期冬季极涡比夏、秋季极涡对我国春季降水的影响更明显,特别是前冬北美区、大西洋欧洲区极涡面积的影响。 相似文献
2.
北极涡活动对我国同期及后期气温的影响 总被引：17，自引：0，他引：17
利用NCEP／NCAR1950-2002年500hPa月平均再分析高度场资料计算出北半球及各分区的月平均极涡面积、强度，讨论了它们与我国气温的相关。结果表明：北半球500hPa年平均和4季的极涡面积大小与我国多数站点同期气温呈负相关，尤其在年平均及冬季状况下最显著，1-12月极涡面积与气温的负相关呈由减弱到增强的变化趋势；而极涡强度与我国同期气温的相关性相对较弱，在秋冬季不少地区出现正相关，1-12月极涡强度与气温负相关性的变化趋势是由增强到减弱。利用奇异值分解研究极涡对后期我国气温的影响后发现，极涡指数与后期我国气温呈负相关，但不同季节差异较大。当冬季Ⅳ区极涡面积显著缩小、北半球极涡总强度明显增强时，长江中下游以北及东北地区下一年春季气温通常上升；春季Ⅰ区极涡面积、强度异常偏大，则夏季华南沿海、西南及河套地区气温比常年偏低；若春季北半球极涡强度减弱、夏季亚洲区极涡面积收缩，则其后的秋季华北气温相对较高。 相似文献
3.
北极涛动、极涡活动异常对北半球欧亚大陆冬季气温的影响 总被引：4，自引：0，他引：4
利用1951-2012年NCEP/NCAR全球月平均500 hPa高度场、气温场等再分析资料,北极涛动（AO）指数,北半球及其4个分区的极涡指数等资料,分析极涡和AO对北半球特别是欧亚大陆冬季气温异常分布的影响。北半球极涡面积指数与北半球气温相关场呈由北向南的“+、-”分布,显著正相关中心位于极区,显著负相关中心位于欧亚大陆中高纬度地区;AO指数与气温的相关场分布与此反位相。极涡各分区面积指数体现与各大洲气温显著相关的地域特征,尤其是亚洲极涡面积指数比AO的相关区域更偏向亚洲和中国东部及沿海地区,能表征亚洲大陆冬季风向中低纬度爆发的某些特征。2006年以来AO指数呈较明显的下降趋势,北半球、亚洲区极涡面积指数呈显著的上升趋势,这是有利于欧亚大陆近几年连续冬季气温异常偏低的年代际背景;2009-2011年北半球欧亚大陆冬季大范围低温事件,不仅与冬季AO负位相明显变强有关（2011年除外）,与北半球以及亚洲区极涡面积指数偏大联系更为密切,亦表明该区域冬季变冷的自然变率明显增强。 相似文献
4.
冬季北极涛动与极涡的变化分析 总被引：11，自引：5，他引：11
利用NCEP／NCAR资料计算出冬季极涡面积（PVA）指数和极涡强度（PVI）指数，对冬季北极涛动（AO）和北半球500hPa极涡指数进行周期分析，讨论了冬季AO与极涡的年际、年代际变化。结果表明：冬季AO指数与PVA指数呈反相关关系，与PVI指数呈正相关关系，且AO指数呈上升趋势，PVA指数呈下降趋势。冬季AO指数、PVA指数以及PVI指数均具有多重周期。强（弱）AO指数年，极地500hPa高度场降低（升高），PVI指数偏大（偏小），PVA指数偏小（偏大）。500hPa高度场上亚洲大槽、北美大槽均减弱（加强）。AO可激发出类似EU遥相关型的异常，从而影响到东亚地区的气候。冬季AO指数在1982年发生突变，且突变后北太平洋地区的正中心位置更靠东，强度更大。此外，AO突变前后极涡变化不是很显著。 相似文献
5.
北极海冰和北半球500hPa极涡的相互关系 总被引：7，自引：0，他引：7
利用NCEP/NCAR 2.5°×2.5°的500 hPa高度场月平均再分析资料和1°×1°的海冰资料分别计算了北半球500 hPa极涡面积、极涡强度指数和北极海冰面积指数,分析了它们的经向分布、周期变化以及长期变化趋势中的突变。结果表明,海冰和极涡在经向分布上有明显差异,就东西半球而言它们的相对位置也不一样。除了都具有4个月、准半年、准1 a、4~5 a和10 a的共同周期外,还呈现出各自的周期变化。北极海冰面积自20世纪80年代以来呈明显减小趋势,北半球极涡面积也呈减小趋势,但是它们发生突变的时间却完全不同。海冰与极涡面积有显著的正相关关系,但海冰和极涡强度、极涡面积和极涡强度之间的关系却纷繁复杂。 相似文献
6.
夏季北极涡与副热带高压的联系及对华北降水的影响 总被引：19，自引：2，他引：17
由于北极涡与副热带高压是两个影响我国天气气候变化的主要大气环流实体,两者紧密相联,且均对华北夏季降水有明显作用,本文使用NCEP/NCAR再分析资料、国家气候中心提供的74个大气环流因子及中国160 站月降水资料,利用合成分析、相关分析及SVD等方法讨论了夏季北极涡与北半球大气环流及副热带高压的相互关系,分析了夏季北极涡及副高对华北降水的共同作用.结果表明:(1) 北极涡的变化不仅与高纬高度场密切相关,而且与中、低纬度环流紧密联系,当极涡异常偏大偏强,中、低纬地区位势高度均明显偏低,北半球副高的面积和强度易偏小,北界位置易偏南,其中副高强度的变化最大.(2) 各分区极涡因子与副高因子之间基本呈显著的负相关,而与西太平洋和南海副高的北界、脊线位置呈正相关.(3) 极涡指数、副高脊线及北界指数与华北降水之间以正相关为主,副高面积、强度指数与华北降水基本呈负相关.当亚洲和欧洲区极涡异常南扩,北非、大西洋、北美副高显著收缩减弱,西太平洋和南海副高明显北抬时,华北降水易增加. 相似文献
7.
利用NCEP/NCAR再分析资料,统计了近50年500,300,200和100 hPa等压面上北半球及4个分区冬季极涡面积和强度指数,并讨论了各层等压面上不同区域极涡面积比例变化特点和500 hPa极涡中心位置变化特征,揭示了冬季各层极涡之间同期和滞后关系,分析了冬季极涡面积与中国平均温度和极端气温的关系。结果表明:(1)北半球极涡面积、强度均经历了先扩张后收缩的变化,20世纪80年代中后期气候变暖以后4层等压面上发生了极涡面积缩小,90年代中期发生强度减弱的年代际突变,只是较面积变化而言,强度年代际变化较弱,极涡面积和强度在年代际上相关显著。(2)位于平流层低层(100 hPa)的极涡年平均面积、强度最大,并且随季节变化幅度也是最大,尤以Ⅰ区(亚洲大陆区)、Ⅳ区(大西洋欧洲大陆区)更为显著。就年内变化而言,100 hPa极涡面积极大值的出现落后于其他层,极小值的出现又早于其他层,并且冬季前期100 hPa极涡面积对其后期500,300和200 hPa的变化有一定影响。(3)4层极涡面积都偏离Ⅳ区,500 hPa极涡基本偏向Ⅱ区(太平洋区)、Ⅲ区(北美大陆区),300,200和100 hPa偏向Ⅰ、Ⅱ区,500 hPa极涡中心多位于Ⅱ区或Ⅲ区。(4)在全球变暖背景下,近50年中国冬季平均气温、暖日(夜)呈现明显的增加趋势,冷日(夜)呈明显的减少趋势,并且突变都发生在20世纪80年代中期。(5)中国冬季平均气温、极端气温指数与极涡面积相关关系以500hPa最为显著。分区来看与500 hPaⅠ区相关最为明显,300 hPaⅠ区、200 hPaⅠ区和100 hPaⅣ区次之。极涡从平流层低层(100 hPa)到对流层中层(500 hPa)是从IV区到I区逐渐影响中国冬季气温。(6)500 hPaⅠ区极涡面积的扩大有利于除东北以外中国大部分地区冷日/夜(暖日/夜)次数的增加(减少),而100 hPaⅢ、Ⅳ区、500 hPaⅣ区面积的扩大有利于中国北方大部分地区冷日/夜(暖日/夜)次数增加(减少),且极涡面积与冷(暖)夜的相关系数要高于与冷(暖)日的,与冷日(夜)的相关系数要好于与暖日(夜)的。 相似文献
8.
华北地区低云量的变化特征及其影响因子分析 总被引：2，自引：0，他引：2
利用1961—2005年华北地区42个测站月平均低云量资料,采用趋势分析、Morlet小波分析等方法分析了华北地区四季低云量的年际变化和周期特征,并利用奇异值分解方法研究了秋季华北地区低云量与500hPa环流指数的关系,重点分析了西太平洋副热带高压(下称西太副高)面积如何影响秋季华北地区低云量变化。结果表明,近45年华北地区四季低云量减弱趋势显著,以秋季减少最多;在年代际尺度上华北地区四季低云量均存在准16年周期,夏季低云量在年际尺度上有显著的准2～4年周期特征;秋季华北地区低云量主要受西太副高面积指数、强度指数、Ⅰ区极涡面积指数、Ⅱ区极涡强度指数和北半球极涡强度指数影响;当秋季西太副高面积偏大(小)时,华北地区上空500hPa高度场偏高(低),上升运动减弱(增强),850hPa南风减小(增大),低层经向水汽输送随之减弱(增强),并且可降水量减少(增大)不利于(有利于)低云的生成;极涡主要是通过影响低层经向风,进而影响华北地区低云量。 相似文献
9.
南亚高压的年际和年代际变化 总被引：56，自引：10，他引：56
利用1958～1998年NCEP/NCAR再分析月平均100 hPa高度场和风场资料， 依据大气环流观测事实及天气学原理，较客观地定义了描述南亚高压活动的特征参数， 然后对南亚高压的年际及年代际变化特征进行了系统的诊断分析。发现北半球中低纬 100 hPa环流异常具有空间整体性和时间持续性，即北半球中低纬100 hPa环流同时加 强或同时减弱，并且其整体异常具有明显的年代际变化。南亚高压面积和强度的变化 存在3.8年的振荡周期，与ENSO的循环周期一致。南亚高压的中心和脊线在夏季较为稳 定，较大的年际差异出现在春季。高压面积和强度的年际变化最明显，并且面积大、 强度强的年份往往与El Niao年相对应。南亚高压的位置和强度还存 在明显的年代际变化，自1978年以后，冬半年南亚高压脊线南移，中心东移，面积增大， 强度增强，夏半年南亚高压的位置变化不很明显，但是面积和强度也增大增强。这种年代 际异常与低层大气系统及赤道太平洋海温的年代际异常一致。南亚高压强度距平与热带 海洋SSTA密切相关，与印度洋海区的同期相关最好。南亚高压强度异常对印度洋SSTA的 响应时间为0～5个月，对赤道中东太平洋SSTA的响应时间为4～6个月。南亚高压明显的 年际和年代际变化特征表明，可将南亚高压看作气候系统中大气子系统异常的强信号， 通过分析南亚高压的年际及年代际异常可以更直接地研究和预测区域气候异常。 相似文献
10.
平流层极涡变化与我国冬季气温、降水的关系 总被引：1，自引：0，他引：1
利用国家气候中心提供的1951-2010年逐月环流指数资料,分析了北半球极涡强度指数、面积指数和中心强度指数的相关关系,并通过极涡强度指数的变化讨论了冬季北半球极涡强度的时间变化特征。结果表明,冬季极涡强度指数与面积指数和中心强度指数有较好的相关性,能够更好地反映冬季极涡强度的变化特征;冬季极涡存在准13年的年代际振荡周期,准5年的年际振荡周期在20世纪90年代后期较为明显。结合气温、降水观测资料和NCEP/NCAR月平均再分析资料,探讨了极涡强、弱不同年份我国冬季气温、降水和大气环流形势的变化。相对极涡弱值年而言,极涡强值年我国北方地区、东部地区特别是东北地区的气温偏高,西南大部分地区的气温偏低,长江流域和华南地区的气温变化不明显;我国南方地区降水偏多,长江中下游和华南地区的降水偏多最为明显,北方地区的降水略有减少;500hPa高度场上高纬度地区的位势高度降低,中高纬度的位势高度升高,冷空气向极地聚集,东亚大槽减弱,我国东北和东部地区的气温偏高;同时东亚冬季风减弱,湿空气向我国内陆输送,长江流域和我国南方地区的降水偏多。 相似文献
11.
2019-2020冬季北极平流层极涡异常并且持续的偏强,偏冷.利用NCEP再数据和OMI臭氧数据,本文分析了此次强极涡事件中平流层极涡的动力场演变及其对地面暖冬天气和臭氧低值的影响.此次强极涡的形成是由于上传行星波不活跃.持续的强极涡使得2020年春季的最后增温出现时间偏晚.平流层正NAM指数向下传播到地面,与地面AO指数和NAO指数相一致,欧亚大陆和北美地面气温均比气候态偏暖,在欧亚大陆的一些地区,2020年1月和2月的气温甚至偏高了 10K.2020年2月以来北极臭氧出现了2004年以来的最低值,2020年3-4月60°-90°N的平均臭氧柱总量比气候态偏低了 80DU. 相似文献
12.
Alaskan Arctic waters have participated in hemispheric-wide Arctic warming over the last two decades at over two times the rate of global warming. During 2008–13, this relative warming occurred only north of the Bering Strait and the atmospheric Arctic front that forms a north–south thermal barrier. This front separates the southeastern Bering Sea temperatures from Arctic air masses. Model projections show that future temperatures in the Chukchi and Beaufort seas continue to warm at a rate greater than the global rate, reaching a change of +4℃ by 2040 relative to the 1981–2010 mean. Offshore at 74°N, climate models project the open water duration season to increase from a current average of three months to five months by 2040. These rates are occasionally enhanced by midlatitude connections. Beginning in August 2014, additional Arctic warming was initiated due to increased SST anomalies in the North Pacific and associated shifts to southerly winds over Alaska, especially in winter 2015–16. While global warming and equatorial teleconnections are implicated in North Pacific SSTs, the ending of the 2014–16 North Pacific warm event demonstrates the importance of internal, chaotic atmospheric natural variability on weather conditions in any given year. Impacts from global warming on Alaskan Arctic temperature increases and sea-ice and snow loss, with occasional North Pacific support, are projected to continue to propagate through the marine ecosystem in the foreseeable future. The ecological and societal consequences of such changes show a radical departure from the current Arctic environment. 相似文献
13.
Mechanism of an Abrupt Decrease in Sea-Ice Cover in the Pacific Sector of the Arctic during the Late 1980s 总被引：1，自引：0，他引：1
Jianfen Wei 《大气与海洋》2014,52(5):434-445
The recent decline in Arctic sea-ice cover (SIC) shows seasonal and regional characteristics. The retreat of summer sea ice has occurred mainly in the Pacific sector of the Arctic. In this study, using the moving t-test, we found an abrupt change event in the long-term sea-ice area in the Pacific sector in summer 1989. This event was linked to the phase shift of the Arctic Oscillation (AO) or the Northern Annular Mode (NAM). Corresponding with the AO/NAM phase shift from negative to positive, the area of the northern hemisphere stratospheric polar vortex decreased abruptly in winter 1988/89. Comparisons of two periods before (1979–1988) and after (1989–1993) the abrupt decrease in sea ice show that an anomalous winter sea level pressure (SLP) was induced by changes in the polar vortex leading to an anomalous cyclonic ice drift in the Pacific sector. The changes in SLP and wind field persisted into the following spring, resulting in a decrease in SIC and warming of the surface air temperature (SAT). The influence of the spring SLP and SAT on ice persisted into the following summer. Meanwhile, the increased summer net surface heat flux over the ocean and sea ice as a result of the decreased spring ice cover further contributed to the summer sea-ice melt. 相似文献
14.
We investigated the differences between stratospheric (S-type) and tropospheric (T-type) Arctic Oscillation (AO) events on the intraseasonal time scale, in terms of their influences on surface air temperature (SAT) over the Northern Hemisphere and the dynamic features associated with their spatial structures. S-type AO events showed a stratosphere-troposphere coupled structure, while T-type events exhibited a stratosphere-troposphere uncoupled structure. The annular SAT anomalies over the Northern Hemisphere were found to be associated with S-type AO events, whereas such an annular feature was substantially destructed in T-type AO events. The different horizontal structures in the troposphere of the two types could mainly be attributed to transient eddy feedback forcing. As for the vertically uncoupled structure of Ttype events, the underlying dynamical features that differentiate them from S-type events lie in the vertical propagation of zonally confined Rossby waves. In T-type events, the zonally confined Rossby wave packets can emanate from the significant height anomalies over Northeast Asia, where one vertical waveguide exists, and then propagate upward into the stratosphere. In contrast, such a vertical propagation was not evident for S-type events. The stratospheric anomalies associated with the upward injection of the zonally confined Rossby waves from the troposphere in T-type events can further induce the anomalous vertical propagation of planetary waves (PWs) through the interference between the climatological-mean PWs and anomalous PWs, leading to the final stratosphere-troposphere uncoupled structure of T-type events. 相似文献
15.
In this paper,the dynamical evolutions of two types of Arctic Oscillation (AO),the stratospheric (S) and tropospheric (T) types,have been investigated on an intermediate time scale in terms of transient eddy feedback forcing and three-dimensional Rossby wave propagation.S-Type (T-type) events are characterized by an anomalous stratospheric polar vortex that is in phase (out of phase) with its tropospheric counterpart.Approximately onethird of AO events,both positive and negative,are T-type events.For the positive phase of a T-type event,the formation and maintenance of stratospheric positive anomalies over the polar cap are associated with an upward propagation of Rossby wave packets originating from the near-tropopause altitude over northeastern Asia.However,such upward propagating features are not found for S-type events.In the troposphere,transient eddy feedback forcing is primarily responsible for the meridional seesaw structure of both the S-and T-type events,with an additional contribution from Rossby wave propagation. 相似文献
16.
Pavel Vargin 《大气与海洋》2015,53(1):29-41
AbstractThe 2009–10 Arctic stratospheric winter, in comparison with other recent winters, is mainly characterized by a major Sudden Stratospheric Warming (SSW) in late January associated with planetary wavenumber 1. This event led to a large increase in the temperature of the polar stratosphere and to the reversal of the zonal wind. Unlike other major SSW events in recent winters, after the major SSW in January 2010 the westerlies and polar vortex did not recover to their pre-SSW strength until the springtime transition. As a result, the depletion of the ozone layer inside the polar vortex over the entire winter was relatively small over the past 20 years. The other distinguishing feature of the 2010 winter was the splitting of the stratospheric polar vortex into two lobes in December. The vortex splitting was accompanied by an increase in the temperature of the polar stratosphere and a weakening of the westerlies but with no reversal. The splitting occurred when, in addition to the high-pressure system over northeastern Eurasia and the northern Pacific Ocean, the tropospheric anticyclone over Europe amplified and extended to the lower stratosphere. Analysis of wave activity in the extratropical troposphere revealed that two Rossby wave trains propagated eastward to the North Atlantic several days prior to the vortex splitting. The first wave train propagated from the subtropics and mid-latitudes of the eastern Pacific Ocean over North America and the second one propagated from the northern Pacific Ocean. These wave trains contributed to an intensification of the tropospheric anticyclone over Europe and to the splitting of the stratospheric polar vortex. 相似文献
17.
Xiangdong ZHANG Yunfei FU Zhe HAN James E.OVERLAND Annette RINKE Han TANG Timo VIHMA Muyin WANG 《大气科学进展》2022,39(4):553-565
Three striking and impactful extreme cold weather events successively occurred across East Asia and North America during the mid-winter of 2020/21.These events open a new window to detect possible underlying physical processes.The analysis here indicates that the occurrences of the three events resulted from integrated effects of a concurrence of anomalous thermal conditions in three oceans and interactive Arctic-lower latitude atmospheric circulation processes,which were linked and influenced by one major sudden stratospheric warming(SSW).The North Atlantic warm blob initiated an increased poleward transient eddy heat flux,reducing the Barents-Kara seas sea ice over a warmed ocean and disrupting the stratospheric polar vortex(SPV)to induce the major SSW.The Rossby wave trains excited by the North Atlantic warm blob and the tropical Pacific La Nina interacted with the Arctic tropospheric circulation anomalies or the tropospheric polar vortex to provide dynamic settings,steering cold polar air outbreaks.The long memory of the retreated sea ice with the underlying warm ocean and the amplified tropospheric blocking highs from the midlatitudes to the Arctic intermittently fueled the increased transient eddy heat flux to sustain the SSW over a long time period.The displaced or split SPV centers associated with the SSW played crucial roles in substantially intensifying the tropospheric circulation anomalies and moving the jet stream to the far south to cause cold air outbreaks to a rarely observed extreme state.The results have significant implications for increasing prediction skill and improving policy decision making to enhance resilience in“One Health,One Future”. 相似文献
18.
On the Differences and Climate Impacts of Early and Late Stratospheric Polar Vortex Breakup 总被引：1，自引：1，他引：0
The stratospheric polar vortex breakup (SPVB) is an important phenomenon closely related to the seasonal transition of stratospheric circulation. In this paper, 62-year NCEP/NCAR reanalysis data were employed to investigate the distinction between early and late SPVB. The results showed that the anomalous circulation signals extending from the stratosphere to the troposphere were reversed before and after early SPVB, while the stratospheric signals were consistent before and after the onset of late SPVB. Arctic Oscillation (AO) evolution during the life cycle of SPVB also demonstrated that the negative AO signal can propagate downward after early SPVB. Such downward AO signals could be identified in both geopotential height and temperature anomalies. After the AO signal reached the lower troposphere, it influenced the Aleutian Low and Siberian High in the troposphere, leading to a weak winter monsoon and large-scale warming at mid latitudes in Asia. Compared to early SPVB, downward propagation was not evident in late SPVB. The high-latitude tropospheric circulation in the Northern Hemisphere was affected by early SPVB, causing it to enter a summer circulation pattern earlier than in late SPVB years. 相似文献