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1.
两个大气环流模式SAMIL和BCC_AGCM对北半球冬季极涡振荡的模拟对比 总被引:1,自引:1,他引:1
基于与NCEP再分析资料的比较, 本文利用大气环流模式SAMIL和北京气候中心大气环流模式BCC_AGCM的1950~1999年的AMIP试验模拟数据, 对北半球冬季环流及平流层极涡振荡的模拟性能进行了评估分析。结果表明两个模式都可以再现北半球环流基本型以及环流振荡的主导模态。对冬季气候平均态的模拟, 两个模式模拟的热带—热带外温度梯度均偏大, 极夜急流偏强, 极涡偏冷偏强;100~20 hPa平均位势高度场谐波分析表明两个模式模 拟的行星波偏弱;气候平均的10 hPa极夜急流均存在1个月的季节漂移, 200 hPa副热带西风急流较NCEP偏弱。两个模式模拟的环流变化的主导模态均代表极涡振荡, SAMIL极涡振荡的强度大于BCC_AGCM, BCC_AGCM极涡振荡的频率要高于SAMIL。连续功率谱分析表明, NCEP资料中极涡振荡存在4.6个月的显著周期, 相应地, SAMIL中为5.5个月的显著周期, BCC_AGCM中为4.8个月。NCEP资料中的极涡振荡主要发生在12~3月, SAMIL模拟的极涡振荡主要发生在2~3月, BCC_AGCM模拟的极涡振荡主要发生在2~4月。 相似文献
2.
北半球冬季行星波的传播及其输运作用 总被引:20,自引:0,他引:20
利用变换欧拉平均方程讨论了行星波动力学。观测和模拟结果都表明,在北半球冬季准定常行星波的经向传播存在两支波导。一支为高纬度波导,另一支则为低纬度波导。这些结果与理论分析相当一致。通过对EP通量进一步的研究表明,平流层爆发性增温是沿高纬度波导传播的异常行星波与平均气流相互作用的结果。而热带风场的准两年周期振荡(QBO)是低纬度平流层下层大气纬向平均流的一个重要年际变化,它可以影响行星波沿低纬度波导的传播;此外,由一个行星波一平均流耦合模式模拟的结果表明,这个热带风场的变化还可以通过波流相互作用调制行星波沿高纬度波导的传播。 行星波对臭氧的输运作用在文中也进行了分析。行星波强迫出的剩余平均环流表明,耗散的行星波有强的输运作用;向北的涡动热量输送可以强迫出一个正的输运环流,其在低纬度上升并在高纬度下沉。同时研究还表明,热带风场的QBO对行星波传播的调制对输运环流也有重要影响,模式结果表明,在QBO的东风位相期间行星波引起的输运作用明显增强,其结果可用于解释平流层高纬度臭氧的年际变化。 相似文献
3.
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
4.
Northern Hemisphere Stratospheric Polar Vortex Extremes in February under the Control of Downward Wave Flux in the Lower Stratosphere 下载免费PDF全文
《大气和海洋科学快报》2012,(3):183-188
Using ECWMF ERA-40 and Interim reanalysis data, the planetary wave fluxes associated with the February extreme stratospheric polar vortex were studied. Using the three-dimensional Eliassen-Palm (EP) flux as a measure of the wave activity propagation, the authors show that the unusual warm years in the Arctic feature an anomalous weak stratosphere-troposphere coupling and weak downward wave flux at the lower stratosphere, especially over the North America and North Atlantic (NANA) region. The extremely cold years are characterized by strong stratosphere-troposphere coupling and strong downward wave flux in this region. The refractive index is used to examine the conception of planetary wave reflection, which shows a large refractive index (low reflection) for the extremely warm years and a small refractive index (high reflection) for the extremely cold years. This study reveals the importance of the downward planetary wave propagation from the stratosphere to the troposphere for explaining the unusual state of the stratospheric polar vortex in February. 相似文献
5.
定常行星波的垂直传播及其动力学效应 总被引:2,自引:1,他引:2
本文用一个β平面准地转模式考察了定常行星波在大气中垂直传播的特性,讨论了波的水平尺度和基本气流的结构等对定常行星波垂直传播的影响,指出了高低层大气之间相互作用的特点及条件。 相似文献
6.
涡动在南北半球平流层极涡崩溃过程中作用的比较 总被引:2,自引:1,他引:2
比较了南北半球春季平流层极涡的崩溃过程以及涡动在此崩溃过程中的作用。极涡的崩溃时间以平流层极夜急流核区最后一次西风转换为东风的时间来确定。结果表明南北半球平流层极涡的崩溃过程有着共同的特点,涡动和非绝热加热过程都对极涡的崩溃起着重要的作用,在极涡崩溃前平流层行星尺度波动活动明显,极涡崩溃以后,这种波动活动便迅速减弱。其中从对流层上传的行星波决定着极涡的具体崩溃时间。两个半球的差别主要表现在南半球极涡崩溃过程一般始于平流层高层,然后逐渐下传,而北半球这种下传不是很明显。其次,北半球平流层极涡崩溃偏晚年,极涡的减弱有两次过程,第一次为快速变化过程,第二次变化比较缓慢,而南半球平流层极涡崩溃无论早晚年只有一次减弱过程。长期的变化趋势分析表明南北半球平流层极涡的崩溃时间逐渐推迟,特别是20世纪90年代中后期以来,这种推迟更加明显。进一步的研究还发现,伴随着平流层极涡的崩溃过程平流层和对流层存在强烈的动力耦合,南北半球极涡迅速减弱前,各自半球的环状模指数也由负指数增加为正指数,表明低层环流对于平流层极涡的崩溃起到重要的作用;同时极涡不同强度所对应的低层环状模指数也不同,这可能与不同强度平流层极涡对于上传的行星波的反射有关。 相似文献
7.
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
8.
Interannual variability of the winter stratospheric polar vortex in the Northern Hemisphere and their relations to QBO and ENSO 总被引:1,自引:0,他引:1
We investigated the interannual variations of the winter stratospheric polar vortex in this paper.
EOF analysis shows that two modes of variability dominate the stratospheric polar vortex on interannual
timescales. The leading mode (EOF1) reflects the intensity variation of the polar vortex and is characterized
by a geopotential height seesaw between the polar region and the mid-latitudes. The second one (EOF2) exhibits
variation in the zonal asymmetric part of the polar vortex, which mainly describes the stationary planetary
wave activity. As the strongest interannual variation signal in the atmosphere, the QBO has been shown to
influence mainly the strength of the polar vortex. On the other hand, the ENSO cycle, as the strongest
interannual variation signal in the ocean, has been shown to be mainly associated with the variation of
stationary planetary wave activity in the stratosphere. Possible influences of the stratospheric polar
vortex on the tropospheric circulation are also discussed in this paper. 相似文献
9.
利用1970—2010年NCEP/NCAR再分析资料、我国160站月平均降水资料分析了平流层极涡向欧亚大陆偏移与我国冬季降水的关系。结果表明:1月极涡偏欧亚大陆强度指数与同期1月降水的显著正相关区域主要分布在我国中部大面积地区及新疆西南部的少数地区,显著负相关区域主要分布在新疆中部;相对1月而言,与后期2月显著正相关区域仍然主要分布在我国的中部地区但向西北方向延伸,使得华中北部、华北南部相对减少,而华北西部、西北东部等地区增大。对流层环流形势显示出在欧亚型强极涡年的1月,东亚冬季风和东亚大槽异常减弱,我国内陆中东部东南风距平显著,而贝加尔湖北部北风距平显著,南下的冷空气与暖湿气流交汇地区较常年偏北,同时我国中部地区低层水汽向上传播也明显增强,存在显著的水汽强辐合中心。 相似文献
10.
热带加热异常影响冬季平流层极涡强度的数值模拟 总被引:1,自引:0,他引:1
本文利用大气环流模式SAMIL/LASG,通过选择两种对流参数化方案,研究了热带加热异常对热带外平流层模拟的影响。结果表明,因不同对流参数化方案引起的热带对流加热状况的差异,可显著影响模式对北半球冬季平流层极涡强度的模拟偏差。与采用Manabe对流参数化方案相比,采用Tiedtke参数化方案可以显著改善对平流层极涡强度的模拟,使平流层极涡“过强”及极区“过冷”的模拟偏差得到明显改善。研究其中的影响过程发现,由于Manabe方案最大凝结潜热加热高度过低,在对流层中低层;而Tiedtke方案的最大凝结潜热加热位置在对流层中上层,因而Tiedtke(Manabe)方案时热带大气温度在对流层中上层较为偏暖(偏冷),在平流层低层较为偏冷(偏暖)。自秋季开始,与热带对流层高层温度的暖偏差相联系,热带外对流层高层以及热带平流层低层出现伴随的温度冷偏差;与之对应,平流层中纬度从秋季开始也出现持续的温度暖偏差。另外,随着秋冬季节平流层行星波活动的出现,Tiedtke方案时热带外地区行星波1波的强度也明显强于Manabe方案,使得秋冬季节涡动引起的向极热通量在Tiedtke方案时明显偏强,从而造成了冬季平流层极区温度偏暖、极涡强度偏弱。 相似文献
11.
Middle Stratospheric Polar Vortex Ozone Budget during the Warming Arctic Winter, 2002--2003 总被引:1,自引:0,他引:1
The ozone budget inside the middle stratospheric polar vortex(24-36 km) during the 2002-2003 Arctic winter is studied by analyzing Michelson Interferometer for Passive Atmospheric Sounding(MIPAS) satellite data.A comprehensive global chemical transport model(Model for Ozone and Related Chemical Tracers,MOZART-3) is used to analyze the observed variation in polar vortex ozone during the stratospheric sudden warming(SSW) events.Both MIPAS measurement and MOZART-3 calculation show that a pronounced increase(26-28 DU) in the polar vortex ozone due to the SSW events.Due to the weakening of the polar vortex,the exchange of ozone mass across the edge of the polar vortex increases substantially and amounts to about 3.0× 107 kg according to MOZART-3 calculation.The enhanced downward transport offsets about 80% of polar vortex ozone mass increase by horizontal transport.A "passive ozone" experiment shows that only ~55% of the vertical ozone mass flux in February and March can be attributed to the variation in vertical transport.It is also shown that the enhanced downward ozone above ~32 km should be attributed to the springtime photochemical ozone production.Due to the increase of air temperature,the NOx reaction rate increases by 40%-80% during the SSW events.As a result,NOx catalytic cycle causes another 44% decrease in polar vortex ozone compared to the net ozone changes due to dynamical transport.It is also shown that the largest change in polar vortex ozone is due to horizontal advection by planetary waves in January 2003. 相似文献
12.
北半球冬季准定常行星波的三维传播及其年际变化 总被引:16,自引:17,他引:16
作者回顾了应用叶笃正先生所创立的Rossby波频散理论,来研究准定常行星波在三维大气的能量频散以及在北半球冬季三维大气中的传播规律,并应用NCEP/NCAR再分析资料和由大气环流数值模拟所得的模式资料的40年风场、温度场资料计算了冬季北半球准定常行星波的E-P通量.计算结果表明了北半球冬季准定常行星波在三维大气传播具有沿两支波导的传播特征,这与从理论分析所得的结果相吻合.作者还分析了冬季准定常行星波的E-P通量分布的年际变化,分析结果表明了准定常行星波在北半球冬季三维大气中传播的这两支波导有明显的年际振荡;并且,从冬季准定常行星波的E-P通量辐散辐合的年际变化与北极涛动的年际变化相比较,发现准定常行星波两支波导的年际振荡直接影响着北极涛动(AO),因而说明了准定常行星波活动的年际变化可以影响对流层的气候变化. 相似文献
13.
During a series of flights in the winters 1991/92 to 1994/95 total stratospheric NO2 was measured by means of the DOAS (Differential Optical Absorption Spectroscopy) technique on board a C160 (Transall) aircraft. In an area covering 60°W to 60°E, and 16°N to 86°N, the total stratospheric NO2 was observed to vary markedly with latitude and season (winter and spring). In the mid-winter Arctic vortex extremely low total stratospheric NO2 (< 3.1014/cm2) was always found, generally larger amounts of NO2 occurred outside the vortex in winter and towards the spring both inside and outside the vortex. This behaviour of stratospheric NO2 can be explained by the denoxification of the wintertime polar stratosphere. Ambient to the vortex in mid-winter however, sudden increases of total stratospheric NO2 by about a factor of 3 were observed. These sudden increases in stratospheric NO2 coincide with a change in the wavenumber 2 of the geopotential height at 60°N, which indicates that most likely the events are caused by planetary waves efficiently transporting air masses rich in NOx from lower to higher latitudes. The monitoring of stratospheric NO2, during latitudinal traverses ranging from the Arctic (80°N) to the Subtropics (18°N) in spring also unexpectedly showed a large variability in total stratospheric NO2 at mid-latitudes. Since photochemistry almost certainly can be excluded, it is proposed that the observed variability may be due to the planetary wave activity of the stratospheric surf zone, known to dynamically connect the tropical and the polar stratosphere. 相似文献
14.
本文利用1979~2010年的NCEP再分析资料,通过北半球环状模NAM指数挑选出的强、弱极涡个例,分析了北半球平流层异常变化过程中行星波的演变以及与之相联系的我国天气的变化特征。结果表明,在强极涡事件前,行星波1波会被反射回对流层,极地波导减弱,低纬波导增强,中高纬地区的E-P通量矢量有着从平流层传播到对流层的趋势;强极涡事件后,极地波导增强,低纬波导减弱。在弱极涡事件前,中、高纬度行星波1波沿着极地波导的传播明显增强;弱极涡事件后,极地波导明显减弱。与此对应的我国天气也有明显变化,在强极涡事件前,我国大部分地区温度偏低,南方地区偏湿而新疆西北部和云南西部地区偏干;在强极涡事件后,东亚冬季风进一步增强,冷空气加强南下,南方地区可降水量减少,新疆西北部仍然偏干,而云南大部分地区可将水量增加。在弱极涡事件前,东亚冬季风显著增强,使我国气温偏冷,降水减少,而弱极涡事件后,我国气温明显回升,中、东部地区和新疆西北部地区降水明显增加。 相似文献
15.
利用高分辨率的再分析资料ERA40,分析了纬向平均状态下北半球不同尺度的定常波对西风动量沿经向输送的气候态及其年变化。结果表明,对流层中定常波对西风动量输送最强的区域位于中纬度对流层的中上层,定常波在该区域长年向北输送纬向动量,且输送中心随季节有南北移动和强弱变化。此外,在高纬度地区的对流层中上层以及赤道对流层顶附近还有两个相对较弱的输送中心。前者对西风动量的输送长年向南,其垂直范围从对流层低层一直伸展到平流层下层,中心位置相对固定,强度有明显的季节变化。后者位置也相对固定,但输送方向随季节改变。平流层中定常波对西风动量的输送主要位于中高纬度的平流层中上层,定常波在该区域长年向北输送西风动量,中心位置非常稳定,而强度则随季节变化明显。行星尺度定常波的输送作用与总波动的输送作用非常一致,并在很大程度上决定了波动对动量输送强度的季节变化。天气尺度定常波和10波以上的短波的输送作用主要集中在中纬度对流层的中高层。前者与行星尺度定常波共同决定了该区域内的输送强度,并主导了输送中心的南北移动;后者的作用很小,除夏季外均可以忽略。作者给出的不同尺度定常波对西风动量输送的气候态分布不但可以作为日后研究其年际变化的基础,而且还可以为大气环流模式对大气环流模拟能力的评估提供重要的参考。 相似文献
16.
The impact of La Ni?a on the winter Arctic stratosphere has thus far been an ambiguous topic of research. Contradictory results have been reported depending on the La Ni?a events considered. This study shows that this is mainly due to the decadal variation of La Ni?a's impact on the winter Arctic stratosphere since the late 1970 s. Specifically,during the period1951–78,the tropospheric La Ni?a teleconnection exhibits a typical negative Pacific–North America pattern,which strongly inhibits the propagation of the planetary waves from the extratropical troposphere to the stratosphere,and leads to a significantly strengthened stratospheric polar vortex. In contrast,during 1979–2015,the La Ni?a teleconnection shifts eastwards,with an anomalous high concentrated in the northeastern Pacific. The destructive interference of the La Ni?a teleconnection with climatological stationary waves seen in the earlier period reduces greatly,which prevents the drastic reduction of planetary wave activities in the extratropical stratosphere. Correspondingly,the stratospheric response shows a less disturbed stratospheric polar vortex in winter. 相似文献
17.
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
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在对逐日气象资料进行纬向谐波分析的基础上, 对比和讨论了2007/2008年冬季强极涡期间和2008/2009冬季弱极涡期间平流层和对流层不同波数的行星波的变化特征, 特别关注强极涡或弱极涡发生之后, 500 hPa 沿60°N和30°N行星波1波和2波振幅和位相的差异, 以及相应的500 hPa位势场的差异, 进而讨论为什么不同的平流层极涡异常会对东亚有不同的影响, 特别讨论为什么同一种极涡异常, 对我国南北方近地面气温的影响会不同。结果表明:平流层极涡发生异常时, 平流层行星波活动有明显的异常。随着极涡异常的下传, 对流层行星波的振幅和位相也有明显的变化, 而且, 对于不同的纬度带, 其变化又有不同, 表现为:2008年1月强极涡发生之后, 500 hPa行星波1波和2波的扰动都向南伸, 而2009年1月的弱极涡(SSW)期间和之后, 1波和2波的扰动都偏北; 在对流层, 强极涡和弱极涡发生之后不但行星波1波和2波的振幅有所差异, 其位相也有明显的不同。特别是, 其位相的差异还随纬度而变化。就同一年(或者说对于同是强极涡或者同是弱极涡)而言, 无论是1波还是2波, 在60°N和30°N附近的扰动相比, 几乎反位相。这样就使得它们的500 hPa 位势场也有明显不同:在东半球, 主要表现为乌拉尔高压和东亚大槽的强度和位置不同。2008年1月强极涡发生之后, 乌拉尔高压和东亚大槽东移, 不利于冷空气向欧亚大陆北部(包括我国北方)的输送, 使这些地区的温度偏高;而2009年1月弱极涡之后, 东亚大槽西退, 利于冷空气向欧亚大陆北部输送, 导致这些地区较冷。对于同一种极涡异常(如2008强极涡或者2009弱极涡)由于南方和北方行星波扰动的位相不同, 对南方和北方冷暖空气的输送也就不一样。所以同一种极涡异常对(我国)南北地区的温度影响是不同的。 相似文献
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北半球准定常行星波气候平均态的资料分析和数值模拟 总被引:1,自引:1,他引:1
利用NCEP/NCAR再分析资料和大气环流模式(CCSR/NIES AGCM Ver 5.6),对北半球准定常行星波的气候平均态分布进行分析和模拟.再分析资料分析的结果表明:北半球冬季,准定常行星波沿两支波导向上传播,其中一支在对流层上层转向中低纬度传播,另外一支折向高纬度,通过极地波导上传到平流层.其中,1波和2波可以上传到平流层,因而其振幅分布除在中低纬的对流层上层出现一个次大值外,在高纬度平流层中上层会出现一个最大值,3波则主要限制在对流层,其振幅分布除在副热带对流层上层出现一个次大值外,最大值出现在中纬度对流层上层.北半球夏季,整个平流层为东风环流,极地波导不存在,行星波不能上传到平流层,在对流层活动也较弱,1波、2波、3波的传播情况大致相似,表现为在对流层上层由中纬度向赤道地区的传播.相应的振幅分布是,对1波和2波而言,最大值出现在中低纬对流层顶附近,同时在中高纬对流层上层出现一个次大值,而3波的振幅分布正好相反,最大值出现在中高纬对流层上层,次大值则在中低纬对流层顶附近.利用大气环流模式进行的数值模拟表明,模式可以比较好地模拟冬夏季准定常行星波的传播路径,但模拟的北半球冬季沿极地波导向平流层的传播明显偏弱,其结果是对1波、2波而言,高纬度平流层中上层的振幅最大值明显小于再分析资料的数值.文中还讨论了数值模拟与资料分析中行星波的差异可能对大气环流模拟的影响. 相似文献