共查询到20条相似文献，搜索用时 847 毫秒
1.
平流层准两年变化对南海夏季风影响机制的探讨 总被引：2，自引：0，他引：2
利用美国大气研究中心(the National Center for Atmospheric Research, NCAR)的中层大气模式模拟了平流层准两年振荡(Quasi-Biennial Oscillation, QBO)过程对对流层顶和对流层上层的影响, 并结合NCEP(the National Centers for Environmental Prediction)/NCAR、欧洲中期天气预报中心(European Centre for Medium-Range Weather Forecasts, ECMWF)月平均的风场资料和实际的探空观测资料, 分析了平流层QBO对南海夏季风的影响作用. 结果表明: 平流层QBO会引起平流层的异常经向环流并向下传播, 在QBO位相的中后期和位相转换期影响到对流层顶和对流层上层, 使热带和低纬度的对流层上层形成异常的经向气压梯度, 最终在夏季的对流层热带地区激发出不同类型的异常环流—西风位相时, 激发出与南海夏季风环流相反的异常环流, 在南海地区有显著的异常下沉运动, 对南海夏季风有削弱作用; 东风位相时, 激发出反Hadley环流型的异常环流, 在南海地区有明显的异常上升气流, 对南海夏季风有加强的效果. 虽然QBO对南海夏季风经向环流有影响, 但它并不是决定南海夏季风准两年变化的唯一因子. 相似文献
2.
夏季平流层盛行强东风,Rossby波能量难以从对流层向上传播至平流层,而冬季平流层盛行西风,Rossby波能量容易上传,因此以往对Rossby波能量向平流层传播的研究多考虑冬季的情况.而事实上,因为夏季高原上空南亚高压反气旋环流,并非只有强东风存在,所以Rossby波能量也可能在南亚高压区向上传播,从而影响平流层的温度、风场及大气成分等.因此,本文利用ERA-interim逐日再分析资料,分析了1979—2015年夏季南亚高压区Rossby波能量穿越对流层顶传播的特征与机制.结果表明:Rossby波能量可以从南亚高压西北部的窗口区上传至平流层,最高可到达平流层顶,而在南亚高压的其他部分,Rossby波能量均不能穿越对流层顶上传或穿越对流层顶后无法继续上传.南亚高压西北区Rossby波能量可以穿越对流层顶传播的原因是盛行西风,且西风急流出现的频率很小,同时涡动热量通量异常引起的垂直分量的第一项对其上传有很大贡献.南亚高压东北区也盛行西风,然而Rossby波能量不能向上穿越对流层顶的原因是强西风出现频率较高,且温度脊与高度脊位相相近,不利于上传.南亚高压南部均盛行东风,在平流层中下层均为稳定层结,因此Rossby波能量很难上传.南亚高压西南区在对流层位于青藏高原环流的伊朗高原下沉区附近,层结稳定,并且温度脊超前于高度脊,所以Rossby波能量很难上传.而南亚高压东南区在对流层位于南海-西太平洋热带幅合带,层结不稳定,存在Rossby波能量较弱的上传,达到对流层顶后无法继续上传,该区域温度脊落后于高度脊的温压场配置也为Rossby波能量在对流层内的传播提供了条件. 相似文献
3.
分析了1993年到2002年10年间HALOE卫星资料的热带平流层水汽年际变率,结果表明：热带平流层水汽混合比在2~5 hPa、10~30 hPa、30~100 hPa有三组显著的准两年周期振荡（QBO）现象;其中2~5 hPa和10~30 hPa水汽QBO呈反位相循环;30~100 hPa水汽QBO有显著上传特性.SOCRATES3模式模拟和诊断结果表明,热带平流层水汽QBO是在纬向风QBO强迫下产生的次级动力、热力因子和化学作用耦合后的结果：上层主要是环流输送引起,中层是环流输送和温度扰动驱动下的化学作用引起,下层是对流层顶水汽冻结层的温度扰动和环流输送引起. 相似文献
4.
青藏高原和热带西北太平洋大气热源在亚洲地区夏季平流层-对流层水汽交换的年代际变化中的作用 总被引：5，自引：0，他引：5
利用欧洲中期天气预报中心ERA40资料,借助Wei诊断模式研究平流层一对流层水汽交换过程,重点分析亚洲地区夏季平流层．对流层水汽交换的年代际特征,探讨青藏高原和热带西北太平洋大气热源在其变化中的作用．气候学特征表明,北半球夏季“亚洲南部半岛-印度洋-太平洋交汇区”为全球最强的对流层向平流层输送的通道,它能将亚洲季风区丰富的水汽源源不断地输送到平流层,影响平流层水汽的分布和变化．北半球夏季亚洲地区穿越对流层顶水汽交换整体上都具有明显的年代际变化,且在近44a可以分为三段比较稳定的时段：1958～1977年、1978～1992年和1993。2001年．在这三个时段中,孟加拉湾．东亚大陆及南海海域的水汽交换通道作用在逐渐减弱,而西北太平洋地区在水汽交换中扮演着越来越重要的角色．进一步研究发现,青藏高原、热带西北太平洋热源的年代际异常是亚洲地区平流层．对流层水汽交换年代际变化的主要原因．44a来青藏高原和热带西北太平洋的热力作用均发生了重大调整,在年代际尺度上两者的综合作用决定了亚洲夏季风的年代际变异,从而影响平流层．对流层水汽交换的年代际异常．然而不同时段不同地区两者的贡献有所不同,尤其是1992年以后,高原热源影响明显减弱,而热带西北太平洋热源在影响平流层．对流层水汽交换中起主要作用．这些结果对深入认识其他大气成份输送过程和正确评估人类活动（排放）对全球气候的影响也具有重要的指示意义． 相似文献
5.
本文通过分析1957~2002年平流层爆发性增温(SSW)的环流特征,研究平流层爆发性增温可能对我国天气气候的影响.平流层爆发性增温发生后平流层高纬地区有异常的环流变化,但是这种变化并不仅局限于平流层内部,其产生的环流异常能够向下传播,并对对流层的天气和气候产生影响.研究发现,平流层出现强爆发性增温后,平流层异常温度场和位势高度场在中、高纬度形成AO型振荡并向下传播,使得对流层低层西伯利亚高压增强、阿留申低压加深,500 hPa东亚大槽加深且偏西,导致东亚冬季风增强,我国北部大部分地区气温偏低.而在爆发性增温前,强行星波扰动使得东亚大槽加深,西伯利亚高压和阿留申低压同时增强,也可能导致东亚冬季风偏强.El Nio可能激发出强行星波,有利于强SSW事件的发生.通过上述的两个过程可能造成东亚冬季风的加强,这将会对"El Nio事件通过对流层过程而引起东亚冬季风减弱"的结论有一定影响. 因此,ENSO事件影响东亚冬季风及中国的天气气候存在不止一种途径,具体影响情况应该是几种途径的综合结果. 相似文献
6.
2009/2010年冬季北极涛动异常及其影响分析 总被引：1，自引：0，他引：1
2009/2010年冬季出现了持续的北极涛动（AO）负异常,同时北半球的天气气候也发生了大范围的异常,两者的关系是大家极为关注的重要问题.本文的分析表明2009/2010年冬季北半球经历了两次显著的AO负异常过程,2009年12月和2010年2月AO指数分别达到了同期历史的最低值.2009年12月的AO负异常过程又可以又分为两个阶段,第一个阶段是由于前期行星波上传的增强导致平流层极涡减弱,随后平流层环流异常向下发展造成了对流层的AO负异常;第二个阶段是因为对流层低层高纬地区的温度正异常维持了第一个阶段在对流层高纬地区的位势高度正异常,使得AO负异常得以较长时间维持,这两个阶段的接连发生和共同作用使得对流层低层经历了一个较强的AO负异常过程.而2010年2月的AO负异常过程则是由平流层爆发性增温所造成的平流层异常环流下传造成的.通过对历史上11个AO负异常事件的统计分析,可以认为AO负异常事件可能由平流层爆发性增温以及平流层极区弱的环流异常下传造成,也可能来源于对流层内部的动力过程.进一步研究表明,2009/2010年冬季持续的极端AO负异常与该冬季北半球大范围的温度和降水异常有密切联系,关注AO异常及其影响是天气预报、气候预测的重要问题. 相似文献
7.
青藏高原为亚洲季风区的典型代表区域,研究其水汽进入平流层的过程和机理对认识全球气候和大气环境变化具有一定的现实意义. 本文基于中尺度气象模式(WRF)的模拟输出结果(2006年8月20日至8月26)驱动拉格朗日大气输送模式FLEXPART,通过追踪并解析气块的三维轨迹以及温度、湿度等相关物理量的相关变化特征,初步分析了夏季青藏高原地区近地层-对流层-平流层的水汽输送特征. 研究结果表明,源于高原地区近地层的水汽在进入平流层的过程中受南亚高压影响下的大尺度环流和中小尺度对流的共同影响.首先,在对流抬升作用下,气块在短时间内(24 h)可抬升到9~12 km的高度,然后在南亚高压闭合环流影响下,相当部分气块在反气旋的东南侧穿越对流层顶进入平流层中,并继续向低纬热带平流层输送,进而参与全球对流层-平流层的水汽循环过程. 在对流抬升高度上气块位置位于高原的西北侧,然而气块拉格朗日温度最小值主要分布于高原南侧,两个位置上气块的平均位温差值可达15~35 K,这种显著的温度差异将导致气块进入平流层时"脱水". 比较而言,夏季青藏高原地区近地层水汽进入平流层的多寡主要和大尺度汽流的垂直输送有关,而深对流的作用相对较弱. 相似文献
8.
亚洲地区是物质由对流层向平流层输送的主要通道,在平流层-对流层交换中扮演着积极的角色. 本文主要利用卫星资料和欧洲中心ERA40再分析资料,借助Wei诊断模式研究亚洲地区夏季上对流层-下平流层(UTLS)水汽分布和平流层-对流层水汽交换特征,重点着眼于水汽交换的年际变化,并探讨其与亚洲夏季风的联系. 结果表明,季风区UTLS水汽较赤道地区偏多,且通过磁带记录信号的传播,可穿越对流层顶影响下平流层水汽的多寡. 夏季平流层-对流层水汽交换表现出明显的年际特征,其年际变化与亚洲季风强弱变化有密切联系,尤其与南亚夏季风的关系更为显著. 在亚洲夏季风影响下,亚洲地区出现异常的大气环流和垂直运动,从而影响平流层-对流层之间水汽的交换. 这些结果对认识其它大气成分的输送过程也具有重要的指示意义. 相似文献
9.
针对LASGBAP发展的耦合系统模式FGOALS-g2和FGOALS—s2,评估了其对热带太平洋沃克环流气候态的模拟能力,在此基础上,分析了沃克环流的变化特征,讨论了沃克环流变化的机理。对20世纪历史模拟结果的分析表明,两个模式均能够合理再现热带太平洋沃克环流气候态分布特征。观测中,过去百年（1900—2004年）和过去55年（1950～2004年）,沃克环流减弱,而近23年（1982～2004年）,沃克环流增强。在三个时间段内,FGOALS-g2模拟的沃克环流均减弱。FGOALS-s2中,过去百年赤道太平洋大气环流减弱,整个热带太平洋大气环流变化不明显;而在过去55年和近23年,模拟的沃克环流均增强。沃克环流变化模拟偏差与模式模拟的内部变率与观测不一致有关。降水与边界层向对流层输送的水汽相平衡的水循环约束关系可以很好地解释沃克环流的变化。FGOALS—g2中,在过去百年、55年和23年间,热带西太平洋降水相对变率（△P／P）增幅小于水汽相对变率（△q/q）增幅、东太平洋冷舌区△P/P增幅大于△q／q增幅,造成沃克环流减弱。FGOALS—s2中,在过去55年及23年间,热带西太平洋对流质量交换增强,东太平洋对流质量交换减弱,使得沃克环流增强。热带太平洋SST变化趋势分布型主导着沃克环流的变化。在过去55年和23年间,FGOALS—g2（FGOALS—s2）中,热带太平洋海表面温度（SST）变化表现为类El Nino（La Nina）型分布,对应沃克环流减弱（增强）。因此,气候系统模式合理模拟沃克环流变化的前提是对热带太平洋SST变化空间型的成功模拟。这一结论得到AMIP试验结果的支持。 相似文献
10.
大尺度海洋环流是海洋能量再分配的基本物理过程之一,研究西太平洋海洋环流在全球气候变暖背景下的多年代变化趋势对理解和预测未来西太平洋气候变化具有重要意义.本文利用最新发布的世界大洋数据集(WOA18)的年代平均水文观测时间序列,计算了1955~2017年间热带西太平洋北赤道流、北赤道逆流、棉兰老流、源地黑潮和新几内亚沿岸潜流的地转流,估算了各支海流的流量及其多年代变化趋势,分离并讨论了温度变化和盐度变化在海流变化中的贡献.结果发现,北赤道流、棉兰老流和新几内亚沿岸潜流在过去60多年中均表现出显著的长期增强趋势,主要是温度变化贡献的,动力高度的变化趋势模态与各西边界流的变化趋势吻合.分析发现,各支海流同纬度西太平洋海域的区域平均纬向风应力可比较准确地刻画各海流流量的年代际变化特征和多年代增强趋势,表明信风强迫在热带西太平洋海洋环流的年代际变化趋势中具有重要作用.本文还讨论了热带西太平洋历史水文观测数据和流量趋势估计中存在的不确定性.由于WOA18数据集比较完整地涵盖了历史上在热带西太平洋获取的水文环境采样数据,因此本文为估计西太平洋大尺度海洋环流的多年代变化趋势提供了重要观测证据. 相似文献
11.
利用气象场的再分析资料和太阳辐射活动资料,对太阳11年周期活动影响北半球冬季(11月~3月)大气环流的过程进行了统计分析和动力学诊断.根据赤道平流层纬向风准两年振荡(QBO)的东、西风状态对太阳活动效应进行了分类讨论,结果表明：东风态QBO时,太阳活动效应主要集中在赤道平流层中、高层和南半球平流层,强太阳活动时增强的紫外辐射加热了赤道地区的臭氧层,造成平流层低纬明显增温,同时加强了南半球的Brewer-Dobson(B-D)环流,引起南极高纬平流层温度增加;而北半球中高纬的环流主要受行星波的影响,太阳活动影响很小.西风态QBO时,太阳活动效应在北半球更为重要,初冬时强太阳活动除了加热赤道地区臭氧层外,还抑制了北半球的B-D环流,造成赤道平流层温度增加和纬向风梯度在垂直方向的变化,从而改变了对流层两支行星波波导的强度;冬末时在太阳活动调制下,行星波向极波导增强,B-D环流逐渐恢复,造成北半球极地平流层明显增温,同时伴随着赤道区域温度的下降. 相似文献
12.
《Journal of Atmospheric and Solar》2002,64(8-11):1229-1240
Continuous wind observations allow detailed investigations of the upper mesosphere circulation in winter and its coupling with the lower atmosphere. During winter the mesospheric/lower thermospheric wind field is characterized by a strong variability. Causes of this behaviour are planetary wave activity and related stratospheric warming events. Reversals of the dominating eastward directed mean zonal winds in winter to summerly westward directed winds are often observed in connection with stratospheric warmings. In particular, the amplitude and duration of these wind reversals are closely related to disturbances of the dynamical regime of the upper stratosphere.The occurrence of long-period wind oscillations and wind reversals in the mesosphere and lower thermosphere in relation to planetary wave activity and circulation disturbances in the stratosphere has been studied for 12 winters covering the years 1989–2000 on the basis of MF radar wind observations at Juliusruh (55°N, since 1989) and Andenes (69°N, since 1998). Mesospheric wind oscillations with long-periods between 10 and 18 days are observed during the presence of enhanced planetary wave activity in the stratosphere and are combined with a reversal of the meridional temperature gradient of the stratosphere or with upper stratospheric warmings. 相似文献
13.
Recent observations suggest that there may be a causal relationship between solar activity and the strength of the winter Northern Hemisphere circulation in the stratosphere. A three-dimensional model of the atmosphere between 10–140 km was developed to assess the influence of solar minimum and solar maximum conditions on the propagation of planetary waves and the subsequent changes to the circulation of the stratosphere. Ultraviolet heating in the middle atmosphere was kept constant in order to emphasise the importance of non-linear dynamical coupling. A realistic thermo-sphere was achieved by relaxing the upper layers to the MSIS-90 empirical temperature model. In the summer hemisphere, strong radiative damping prevents significant dynamical coupling from taking place. Within the dynamically controlled winter hemisphere, small perturbations are reinforced over long periods of time, resulting in systematic changes to the stratospheric circulation. The winter vortex was significantly weakened during solar maximum and western phase of the quasi-biennial oscillation, in accordance with reported 30 mb geopotential height and total ozone measurements. 相似文献
14.
Based on the daily NCEP/DOE reanalysis II data,dates of the boreal spring Stratospheric Final Warming(SFW) events during 1979–2010 are defined as the time when the zonal-mean zonal wind at the central latitudes(65°–75°N) of the westerly polar jet drops below zero and never recovers until the subsequent autumn.It is found that the SFW events occur successively from the mid to the lower stratosphere and averagely from the mid to late April with a temporal lag of about 13 days from 10 to 50 hPa.Over the past 32 years,the earliest SFW occurs in mid March whereas the latest SFW happens in late May,showing a clear interannual variability of the time of SFW.Accompanying the SFW onset,the stratospheric circulation transits from a winter dynamical regime to a summertime state,and the maximum negative tendency of zonal wind and the strongest convergence of planetary-wave are observed.Composite results show that the early/late SFW events in boreal spring correspond to a quicker/slower transition of the stratospheric circulation,with the zonal-mean zonal wind reducing about 20/5 m s-1 at 30 hPa within 10 days around the onset date.Meanwhile,the planetary wave activities are relatively strong/weak associating with an out-of-/in-phase circumpolar circulation anomaly before and after the SFW events in the stratosphere.All these results indicate that,the earlier breakdown of the stratospheric polar vortex(SPV),as for the winter stratospheric sudden warming(SSW) events is driven mainly by wave forcing;and in contrast,the later breakdown of the SPV exhibits more characteristics of its seasonal evolution.Nevertheless,after the breakdown of SPV,the polar temperature anomalies always exhibit an out-of-phase relationship between the stratosphere and the troposphere for both the early and late SFW events,which implies an intimate stratosphere–troposphere dynamical coupling in spring.In addition,there exists a remarkable interdecadal change of the onset time of SFW in the mid 1990s.On average,the SFW onset time before the mid 1990s is 11 days earlier than that afterwards,corresponding to the increased/decreased planetary wave activities in late winter-early spring before/after the 1990s. 相似文献
15.
南极地区重力波活动有大量报道,相对而言,北极地区重力波的研究还很少.本文利用极区Ny-Alesund站点（78.9°N,11.9°E）无线电探空仪从2012年4月1日到2017年3月31日共5年的观测数据,统计分析了北极地区低平流层惯性重力波的特征.观测显示,月平均纬向风在20 km以下盛行东向风,再随着高度增加,逐渐呈现出半年振荡现象.对流层顶高度在5~13 km范围内变化,其月平均高度显示出年循环,最高出现在夏季,约为10 km,最低出现在冬季,约为8.5 km.对流层和低平流层月平均温度都显示出明显的年周期变化,这与中低纬度观测结果有所不同.结合Lomb-Scargle谱分析和矢端曲线方法,估算了准单色惯性重力波参数.个例研究表明,低平流层惯性重力波呈现出远离源区的自由传播性质.统计结果显示,惯性重力波的水平和垂直波长分别集中在50~450 km和1~4 km范围内,本征频率集中在1~2.5倍惯性频率间,这些值都比中低纬度观测值稍小.垂直方向本征相速度主要集中在-0.3~0 m·s-1,而纬向和经向本征相速度集中在-40~40 m·s-1之间.在5年的观测中,大约91.5%的惯性重力波向上传播.在冬季和早春,由于极地平流层极涡活动,激发出向下传播的惯性重力波,因此,向下传播的比例上升到相应月份的20%左右.由于低层大气盛行的东向风的滤波效应,低平流层大部分惯性重力波向西传播.波能量呈现出明显的年周期变化,最大值在冬季、最小值在夏季,与北半球中低纬度观测结果一致,表明北半球重力波活动普遍冬季强、夏季弱. 相似文献
16.
Observations from the Nimbus 6 pressure modulator radiometer (PMR) have been used to estimate monthly mean planetary wave fluxes of heat and momentum in the stratosphere and mesosphere. While the eddy heat fluxes play an important role in the mean meridional circulation of the winter stratosphere they are shown to be less important in the upper mesosphere. Incorporation of the observed momentum fluxes into the Oxford two-dimensional circulation model has shown that they are incapable of providing the momentum transport necessary to balance the zonal flow accelerations induced by the mean meridional motion. Other unspecified transfer processes represented by Rayleigh frictional damping of the zonal fow are shown to dominate. In contrast the observed fluxes in the stratosphere achieve the necessary redistribution of momentum. Moreover their interannual variability profoundly influences the stratospheric circulation, as demonstrated in the model by the use of two different annual sets of observed momentum fluxes. The desirability of calculating the planetary wave behaviour within the model is indicated. 相似文献
17.
Bodil Karlsson Charles McLandress Theodore G. Shepherd 《Journal of Atmospheric and Solar》2009,71(3-4):518-530
Observations of noctilucent clouds have revealed a surprising coupling between the winter stratosphere and the summer polar mesopause region. In spite of the great distance involved, this inter-hemispheric link has been suggested to be the principal reason for both the year-to-year variability and the hemispheric differences in the frequency of occurrence of these high-altitude clouds. In this study, we investigate the dynamical influence of the winter stratosphere on the summer mesosphere using simulations from the vertically extended version of the Canadian Middle Atmosphere Model (CMAM). We find that for both Northern and Southern Hemispheres, variability in the summer polar mesopause region from one year to another can be traced back to the planetary-wave flux entering the winter stratosphere. The teleconnection pattern is the same for both positive and negative wave-flux anomalies. Using a composite analysis to isolate the events, it is argued that the mechanism for inter-hemispheric coupling is a feedback between summer mesosphere gravity-wave drag (GWD) and zonal wind, which is induced by an anomaly in mesospheric cross-equatorial flow, the latter arising from the anomaly in winter hemisphere GWD induced by the anomaly in stratospheric conditions. 相似文献
18.
Y. Hayashi D. G. Golder J. D. Mahlman S. Miyahara 《Pure and Applied Geophysics》1989,130(2-3):421-443
To examine the effects of horizontal resolution on internal gravity waves simulated by the 40-level GFDL SKYHI general circulation model, a comparison is made between the 3° and 1° resolution models during late December. The stratospheric and mesospheric zonal flows in the winter and summer extratropical regions of the 1° model are much weaker and more realistic than the corresponding zonal flows of the 3° model. The weaker flows are consistent with the stronger Eliassen-Palm flux divergence (EPFD).The increase in the magnitude of the EPFD in the winter and summer extratropical mesospheres is due mostly to the increase in the gravity wave vertical momentum flux convergence (VMFC). In the summer extratropical mesosphere, the increase in the resolvable horizontal wavenumbers accounts for most of the increase in the gravity wave VMFC. In the winter extratropical mesosphere, the increase of VMFC associated with large-scale eastward moving components also accounts for part of the increase in the gravity wave VMFC.The gravity waves in the summer and winter mesosphere of the 1° model are associated with a broader frequency-spectral distribution, resulting in a more sporadic time-distribution of their VMFC. This broadening is due not only to the increase in resolvable horizontal wavenumbers but also occurs in the large-scale components owing to wave-wave interactions. It was found that the phase velocity and frequency of resolvable small-scale gravity waves are severely underestimated by finite difference approximations. 相似文献
19.
The zonally averaged UK Meteorological Office (UKMO) zonal mean temperature and zonal winds for the latitudes 8.75°N and 60°N are used to investigate the low-latitude dynamical response to the high latitude sudden stratospheric warming (SSW) events that occurred during winter of the years 1998–1999, 2003–2004 and 2005–2006. The UKMO zonal mean zonal winds at 60°N show a short-term reversal to westward winds in the entire upper stratosphere and lower mesosphere and the low-latitude winds (8.75°N) show enhanced eastward flow in the upper stratosphere and strong westward flow in the lower mesosphere during the major SSW events at high latitudes. The mesosphere and lower thermosphere (MLT) zonal winds acquired by medium frequency (MF) radar at Tirunelveli (8.7°N, 77.8°E) show a change of wind direction from eastward to westward several days before the onset of SSW events and these winds decelerate and weak positive (eastward) winds prevail during the SSW events. The time variation of zonal winds over Tirunelveli is nearly similar to the one reported from high latitudes, except that the latter shows intense eastward winds during the SSW events. Besides, the comparison of daily mean meridional winds over Tirunelveli with those over Collm (52°N, 15°E) show that large equatorial winds are observed over Tirunelveli during the 2005–2006 event and over Collm during the 1998–1999 events. The variable response of MLT dynamics to different SSW events may be explained by the variability of gravity waves. 相似文献
20.
北极地区(60°N～90°N)平流层纬向风和气压场有明显的季节变化,不同高度层季节变化的时间有差异.北极平流层从冬至夏,季节转换从上向下推进,从夏至冬,季节转换从下向上推进.以20 hPa为例,平均而言,4月上旬以前,北极被极涡控制;4月中旬北极地区高压的势力开始超过低压,5月上旬,北极高压正式建立;7月份达到最强,8... 相似文献