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1.
经圈环流对定常波传播的影响 总被引：1，自引：0，他引：1
在一般斜压大气中，基本气流中包含经圈环流时，定常波传播不仅能穿过东风带，而且明显增强。在基流含有经圈环流的情况下，北半球中纬度地形强迫可引起低纬大气的显著响应，这表明经圈环流在中低纬定常响应的相互联系中起着重要作用；北半球中纬度热力强迫可产生类似北半球夏季季风环流的波列分布，这说明经圈环流在夏季季风环流的形成中起着一定的作用；在赤道东太平洋加热强迫情况下，在冬半球可引起ＰＮＡ型的定常波传播波列，而在夏半球却没有明显的ＰＮＡ特征。这表明经圈环流对冬、夏半球的定常波传播路径有着显著的影响。 相似文献
2.
热带海温异常影响夏季环流的机制研究 总被引：1，自引：0，他引：1
利用正压涡度方程模式对赤道东太平洋和赤道西太平洋暖池区海温异常影响夏季大气环流的机制进行了研究,结果表明:太平洋海温异常会对大气环流产生明显的影响,我国上空环流受其直接影响较小,大气对赤道东太平洋海温升高的响应比对西太平洋暖池海温降低响应明显.西太平洋暖池海温降低和赤道东太平洋海温升高都使极涡明显减弱,对中低纬度大气高度场的影响相反.赤道东太平洋海温升高,中低纬度地区槽脊活动表现不明显,而西太平洋暖池海温降低,会使大气高度场产生明显的槽脊扰动.西太平洋暖池海温降低和赤道东太平洋海温升高,会使涡度场、经向风形成沿驻波波列传播的扰动场.西太平洋暖池海温降低和赤道东太平洋海温升高同时发生时,经向风场使北半球所有的地方都产生了扰动(两条波列路径仍然清楚),沿纬圈和经向都呈有规律的正负相间的分布,扰动表现为驻波特征. 相似文献
3.
Based on researches made by the author in recent years, discussion is made of the quasi-40-day oscillation (QDO) nature and its characteristic propagation, with emphasis on the Southern Hemisphere mid-latitude quasi-periodic cold air forcing on the tropical atmosphere quasi-40-day oscillation along with its effect upon the Northern Hemisphere summer monsoon. It is proposed that the interaction between, or lateral coupling of, meridional circulation systems may serve as the mechanism of the oscillation propagation in a meridional direction. 相似文献
4.
本文采用OSU-AGCM动力框架加入牛顿加热项构成的简化大气环流模式,研究澳洲大陆热力强迫与南北半球环流异常的相关关系。本文对不同平衡温度模拟结果的差异(偏差场)进行了分析,探讨某局地热力强迫对全球其它区域环流异常的影响效应.数值试验结果表明,南北半球海陆热力结构有利于两半球行星尺度经向环流的加强及其低纬跨赤道气流的形成:南半球澳洲大陆热力强迫可以通过东、西风带侧向藕合效应,显著地影响北半球中纬西风带急流状况;二维Rossby波能量频散径向传播可能足澳洲热力强迫与北半球常定环流系统的异常变化相关现象的重要成因,且澳洲大陆强迫产生的径向波列路经与PNA、EU型相似. 相似文献
5.
本文与文献[1]相对应,利用一个非线性初始方程谱模式,研究了中、高纬度理想化的大尺度地形以及北半球实际地形的动力强迫作用对于冬季行星尺度的大气定常波的影响。计算结果证实,根据线性模式的数值试验结果所做的定性分析在非线性情形下仍然是成立的,同时,非线性扰动流场也与线性流场有明显的差异,在纬向平场基本气流相对较弱的地区或垂直层次上差异尤为显著。数值试验表明,北半球实际地形强迫的大尺度扰动,在对流层低层以及对流层上部的中、高纬均主要表现出纬向波数为2的行星波,但是在对流层上部的低纬地区3波分量比较明显。中、高纬的大地形动力强迫作用,对于低纬太平洋高空的反气旋和气旋环流的形成有重要的贡献。 相似文献
6.
EFFECT OF PLANETARY AND SYNOPTIC SCALE WAVES IN MAINTAINING MERIDIONAL CIRCULATIONS AT MID AND LOW LATITUDES* 
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下载免费PDF全文 Following Wu and Chen(1989), in terms of the elliptical differential equation with mean meridional stream function, an equation similar in form to that developed by Kuo(1956) and by use of time average statistics of atmospheric circulation in wavenumber domains at the same intervals of time, a study is made of the contribution of the internal forcing of the atmosphere in two space scales to mean meridional circulation. Results show that planetary waves have considerable influence on the intensity of the upper center of the bi-Hadley cell, and, in contrast, synoptic-scale waves exert vital effect on the Ferrel cell, and that in the Northern Hamisphere(NH) such internal forcings by planetary- and synoptic-scale waves are comparable on mean meridional circulations whereas the latter contribute far more than the former in the Southern Hemisphere(SH).Further, in the northern winter(summer) the contribution of heat(angular momentum) transport of planetary waves allows the descending(ascending) branch to occur as far as around 40°N, some kind of effect that makes quite important contribution to the winter(summer) monsoon circulation in eastern Asia. 相似文献
7.
利用1958～1997年NCEP/NCAR一日四次的风场再分析资料,系统地分析了季节平均西风角动量（即u角动量）经向、垂直输送通量及其三个分量（平均经圈环流、定常波、瞬变涡输送通量）的气候特征,特别是讨论了12～2月、6～8月它们与东、西风带、副热带西风急流、极夜急流之间的联系。结果表明:（1）包含纬度因子的角动量通量与动量通量在高纬地区存在显著差别,高纬对流层上部的强动量输送中心在角动量通量中不明显。而u角动量强经向输送主要在中低纬对流层顶附近和冬半球高纬平流层顶附近,副热带西风急流和极夜西风急流均位于u角动量强向极输送中心及其高纬一侧的辐合区中。（2）发现三个输送分量对急流维持的作用随纬度、季节不同。北半球冬季（夏季）的副热带西风急流主要由平均经圈环流（强度相当的定常波和瞬变涡）强经向输送及辐合维持;南半球西风急流全年均由平均经圈环流和瞬变涡旋输送及辐合维持;冬半球中平流层极夜急流主要由定常波、瞬变涡旋输送及其辐合共同维持。（3）热带东风区是牵连角动量（即Ω角动量）的高值区,它主要由平均经圈环流向对流层上部输送;冬半球副热带及中纬西风区存在u角动量垂直输送的切变区,它主要由平均经圈环流和瞬变涡旋完成;热带对流层顶附近有u角动量的定常波弱向下输送。 相似文献
8.
Summary Through the use of a zonal balance model we investigate the properties of the tropical meridional circulation to a range of specified diabatic forcing fields for climatologically observed zonal winds. As in earlier studies, the solutions show that latent heat release away from the equator forces an asymmetric meridional circulation in response the anisotropy in the inertial stability parameter with respect to the meridional location of the forcing. The presence of strong zonal flows appears to play a relatively minor role in determining the magnitude and asymmetry of the meridional circulation, whereas the structure of the diabatic heating, particularly the meridional breadth, proves to be of much greater importance.A dynamic efficiency factor, which provides an analytic measure of the efficacy of diabatic heating at generating zonal kinetic energy, generally exhibits a meridionally symmetric structure except during Northern Hemisphere summer. This asymmetry gives rise to a pronounced sensitivity of zonal kinetic energy generation to the meridional location of ITCZ convection. Further examination of the flow pattern suggests that for zonal flows representative of those over the Indian Ocean during the Northern Hemisphere summer months, meridional displacements of the heating of less than 20° latitude can result in as much as an order of magnitude difference in the rate of kinetic energy generation. Solution of the balance system also implies the existence of a feedback mechanism, between zonally-organized convection and the energetics properties of the large-scale flow, that is highly sensitive to the meridional location of the convection.With 11 FiguresThe National Center for Atmospheric Research is sponsored by the National Science Foundation. 相似文献
9.
Herv�� Douville S. Bielli C. Cassou M. D��qu�� N. M. J. Hall S. Tyteca A. Voldoire 《Climate Dynamics》2011,37(9-10):1783-1798
While organized tropical convection is a well-known source of extratropical planetary waves, state-of-the-art climate models still show serious deficiencies in simulating accurately the atmospheric response to tropical sea surface temperature (SST) anomalies and the associated teleconnections. In the present study, the remote influence of the tropical atmospheric circulation is evaluated in ensembles of global boreal summer simulations in which the Arpege-Climat atmospheric General Circulation Model (GCM) is nudged towards 6-h reanalyses. The nudging is applied either in the whole tropical band or in a regional summer monsoon domain. Sensitivity tests to the experimental design are first conducted using prescribed climatological SST. They show that the tropical relaxation does not improve the zonal mean extratropical climatology but does lead to a significantly improved representation of the mid-latitude stationary waves in both hemispheres. Low-pass filtering of the relaxation fields has no major effect on the model response, suggesting that high-frequency tropical variability is not responsible for extratropical biases. Dividing the nudging strength by a factor 10 only decreases the magnitude of the response. Model errors in each monsoon domain contribute to deficiencies in the model??s mid-latitude climatology, although an exaggerated large-scale subsidence in the central equatorial Pacific appears as the main source of errors for the representation of stationary waves in the Arpege-Climat model. Case studies are then conducted using either climatological or observed SST. The focus is first on summer 2003 characterized by a strong and persistent anticyclonic anomaly over western Europe. This pattern is more realistic in nudging experiments than in simulations only driven by observed SST, especially when the nudging domain is centred over Central America. Other case studies also show a significant tropical forcing of the summer mid-latitude stationary waves and suggest a weak influence of prescribed observed SST in the northern extratropics. Results therefore indicate that improving the tropical divergent circulation and its response to tropical SST anomalies remains a key issue for increasing the skill of extratropical seasonal predictions, not only in the winter hemisphere but also in the boreal summer hemisphere where the prediction of heatwave and drought likelihood is expected to become an important challenge with increasing concentrations of greenhouse gases. 相似文献
10.
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
11.
印度夏季风的年际变异与北半球大气环流的特征 总被引：2，自引：1，他引：2
印度夏季风的年际变异是大范围大气环流相互联系、相互影响的结果。本文应用１９５１—１９８５年印度夏季风资料，选取强季风年４年和弱季风年６年，分别对北半球５００ｈＰａ高度场进行距平合成分析和复自然正交函数（ＣＥＯＦ）分析。结果指出，大西洋和鄂霍次克海阻塞高压的稳定存在以及乌拉尔山低压槽的频繁活动与强印度季风年相联系，而大西洋和鄂霍次克海低压系统的频繁活动以及欧洲阻塞高压的稳定存在与弱印度季风年相联系。印度夏季风强弱不同年份，春季北半球大气环流已经出现了一些不同特征，这对于当年夏季风的强弱和北半球气候异常有预示作用。印度夏季风强弱的不同年份和不同季节，北半球存在极地和赤道低纬位相函数大而中高纬度位相函数小，且扰动由中高纬向极地和赤道方向传播的特征 相似文献
12.
When greenhouse gases are increased in coupled GCM experiments there is both a direct effect and an indirect effect due to changes in the surface conditions. In this study we carry out experiments with a perpetual winter atmosphere only model in order to investigate the influence of changes to the surface conditions (sea surface temperatures, sea-ice and snow amount) on the Northern Hemisphere winter mid-latitude mean sea level pressure response. The surface conditions for the perpetual winter model experiments are prescribed from time averages of the HadCM2 control and greenhouse gas experiments. Forcing the perpetual winter model with the HadCM2 greenhouse gas surface conditions produces a negative mean sea level pressure (MSLP) response across both Northern Hemisphere ocean basins, as was found in the coupled model HadCM2 experiment. Additional PW model experiments show that the sea surface temperature forcing from the HadCM2 greenhouse gas experiment dominates the snow and soil moisture content forcings. The sea-ice forcing from the HadCM2 greenhouse gas experiment reduces MSLP at high latitudes. In the north Pacific region MSLP decreases when the global mean warming is applied to the sea surface temperature forcing field at all open sea points. In the north Atlantic region the increased tropics to mid-latitude meridional sea surface temperature gradient is required for MSLP to decrease. These experiments show that the MSLP response in the Northern Hemisphere mid-latitude storm track regions is sensitive to the non-local sea surface temperature anomaly pattern. 相似文献
13.
Abstract This paper presents the seasonal dependence of the stationary and transient eddies of the GLAS/UMD GCM from a two‐year annual cycle integration. The simulated Northern Hemisphere stationary waves are realistic in winter (below 250 mb) and in spring and fall; in winter a large anomalous ridge over the date‐line is noted above 250 mb. The model does not simulate the winter barotropic trough over eastern Canada. In summer the mid‐latitude stationary waves are poorly simulated (possibly owing to anomalous summer rainfall), but the monsoonal structure in the tropics is captured. The stationary wave field at 500 mb in the Southern Hemisphere is not well simulated, with the range of season‐to‐season variability being much larger than observed. The zonally averaged stationary wave rms is realistic below 200 mb in winter and spring, but is less so in summer and autumn, possibly due to erroneous summertime precipitation. The geographical distributions of 500‐mb transient and band‐pass height rms, of transient 850‐mb heat flux and of 200‐mb momentum flux in the Northern Hemisphere are well simulated except for summer. The latitude‐height dependence of height rms and low‐level transient heat flux is realistic in both summer and winter, but the transient momentum flux is not well simulated in summer. The mid‐level transient heat flux is too strong. The overall pattern of transient activity at 500 mb in the Southern Hemisphere is reasonable in the GCM, although there is too much variability in the eastern Pacific, while the observed peak in rms in the New Zealand sector is displaced eastwards in the GCM. The latitude‐height dependence of transient height rms and transient fluxes of heat and momentum looks quite realistic, and is similar in accuracy to the Northern Hemispheric results. 相似文献
14.
热带大气对单一型赤道非对称热源的响应 总被引：1，自引：0，他引：1
本文采用Gill模式得到了热带大气对单一型赤道非对称热源响应的理论解析通解,从理论上完善了单一型赤道非对称热源激发的赤道非对称的大气响应结果。同时在单一型赤道非对称热源的位置、强度及范围变化对大气响应的影响方面做了详细的研究。当热源中心位置北移,北半球气旋强度增加、位置北移,同时赤道辐合气流减弱而越赤道气流增强;当热源强度增强(减弱),热源激发的大气响应整体增强(减弱),但大气分布型不发生变化;当热源范围不断增大(减小)时,北半球气旋强度增强(减弱)、位置西移(东移)、范围增大(减小),同时越赤道气流增强(减弱)。将上述结论应用于分析孟加拉湾地区海温对夏季风爆发影响的研究,指出当孟加拉湾地区经向最大暖海温位于赤道附近时,其两侧表现为Rossby波响应的Gill型气旋环流,而海温暖轴北移后,其南侧激发出有利于季风爆发的越赤道气流,这是Rossby重力混合波对热源响应的结果。这是上述理论结果的一个很好例证,同时也为孟加拉湾夏季风的爆发给出一种动力学解释。 相似文献
15.
16.
南极海冰首要模态呈现偶极子型异常,正负异常中心分别位于别林斯高晋海/阿蒙森海和威德尔海。过去研究表明冬春季节南极海冰涛动异常对后期南极涛动（Antarctic Oscillation,AAO）型大气环流有显著影响,而AAO可以通过经向遥相关等机制影响北半球大气环流和东亚气候。本文中我们利用观测分析发现南极海冰涛动从5～7月（May–July,MJJ）到8～10月（August–October, ASO）有很好的持续性,并进一步分析其对北半球夏季大气环流的可能影响及其物理过程。结果表明,MJJ南极海冰涛动首先通过冰气相互作用在南半球激发持续性的AAO型大气环流异常,使得南半球中纬度和极地及热带之间的气压梯度加大,在MJJ至JAS,纬向平均纬向风呈现显著的正负相间的从南极到北极的经向遥相关型分布。对流层中层位势高度场上,在澳大利亚北部到海洋性大陆区域,出现显著的负异常,在东亚沿岸从低纬到高纬呈现南北走向的“? + ?”太平洋—日本（Pacific–Japan,PJ）遥相关波列,其对应赤道中部太平洋及赤道印度洋存在显著的降水和海温负异常,西北太平洋至我国东部沿海地区存在显著降水正异常和温度负异常;低纬度北美洲到大西洋一带存在的负位势高度异常和北大西洋附近存在的正位势高度异常中心,构成一个类似于西大西洋型遥相关（Western Atlantic,WA）的结构,对应赤道南大西洋降水增加和南撒哈拉地区降水减少。从物理过程来看,南极海冰涛动首先通过局地效应影响Ferrel环流,进而通过经圈环流调整使得海洋性大陆区域和热带大西洋上方的Hadley环流上升支得到增强,海洋性大陆区域特别是菲律宾附近的热带对流活动偏强,激发类似于负位相的PJ波列,影响东亚北太平洋地区的大气环流,而热带大西洋对流增强和北传特征,则通过激发WA遥相关影响大西洋和欧洲地区的大气环流。以上两种通道将持续性MJJ至ASO南极海冰涛动强迫的大气环流信号从南半球中高纬度经热带地区传递到北半球中高纬地区,从而对热带和北半球夏季大气环流产生显著影响。 相似文献
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运用ＩＡＰＡＧＣＭ模式证实了大气对南极冰异常的强迫遥响应是激发产生全球大气季节内振荡的重要机制,进而着重考察了候平均偏差结果的时间序列,并且通过带通滤波处理,特别分析了响应场中３０～６０ｄ低频振荡的特征及其活动。通过分析发现：大气对南极冰减退的响应是一种具有３０～６０ｄ周期的低频遥响应,并呈现出清楚的二维Ｒｏｓｓｂｙ波列特征;强迫场中的３０～６０ｄ季节内振荡具有着同实际大气中的低频振荡相类似的垂直结构和传播特征。大气响应场中３０～６０ｄ振荡能量在垂直方向上随高度的增加而增加,在纬向上表现出明显的区域性特征,即季节内振荡的最大动能区（由于ＣＩＳＫ机制）分布在大洋内;ＥＵＰ,ＰＮＡ,ＡＳＡ和ＲＳＡ波列可能是全球大气低频扰动传播的主要路径,３０～６０ｄ低频扰动在波列路径上的传播具有很大的一致性和系统性,从而使中高纬和热带地区、以及南北半球的３０～６０ｄ大气振荡相互联系起来,而且可以认为,赤道中太平洋和赤道中大西洋地区是南北半球３０～６０ｄ低频振荡间相互作用和相互联系的重要通道。 相似文献
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基于ERA-Interim再分析资料,借助大气模式CAM4,分析了北半球冬季不同月份的平均大气对巴伦支海不同振幅及不同季节海冰扰动的敏感性,并考察了中高纬度典型大气模态的分布变化情况。结果表明,冬季巴伦支海海冰的减少,会导致湍流热通量异常向上、局地异常变暖及水汽含量的异常升高,且相关异常的强度和范围随着海冰减少幅度的减小而减弱。这种局地响应会通过大气环流调整扩散开来,产生远程影响。具体地,冬季大气环流与欧亚地面温度异常对于不同幅度海冰异常的响应是非线性的,且在不同月份也呈现出不同特征。秋季巴伦支海海冰减少虽未引起局地显著的温度异常,但欧亚大陆温度及环流场异常响应的强度更强、范围更广,这表明秋季海冰可以独立地对冬季中纬度大气产生影响。此外,冬季不同月份西伯利亚高压强度、位置对巴伦支海海冰减少的响应是不同的,北大西洋涛动位相的倾向变化对不同季节、不同振幅海冰减少的响应也不相同。冬季海冰减少时,12月和1月,西伯利亚高压强度更易偏强、位置易偏东,2月则与之相反。与冬季相比,秋季海冰偏少时,西伯利亚高压更易稳定维持在欧亚大陆,晚冬时发生北大西洋涛动负位相的概率增大,但出现极端负位相概率降低。这为了解巴伦支海海冰异常对北半球天气、气候的影响提供了参考。 相似文献
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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
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Analysis of Stationary-Wave Nonstationarity in the Northern Hemisphere 500-hPa Height Field 下载免费PDF全文
下载免费PDF全文 ZHOU Guohu WANG Panxing SHI Ning LI Qiaoping SHE Gaojie 《Acta Meteorologica Sinica》2010,24(3):287-296
In this paper, the concept of stationary-wave nonstationarity is presented and elucidated in the framework of the Lorenz circulation decomposition. This concept indicates the relative magnitude of the zonal nonuniform abnormity to the intensity of stationary waves on the monthly mean scale. Based on the Lorenz circulation decomposition, the nonstationarity degree Ius(Ilus) of the global (local) stationary waves is defined, and then used to analyze the stationary-wave nonstationarity at 30° 60°N, where the intensity of stationary waves at 500 hPa in the Northern Hemisphere, as is well known, is very high. The following findings are obtained: (1) There exist seasonal southward and northward movements in the position of the nonstationarity zones of the global stationary waves. The steady stationary waves occur in midlatitudes (35°-55°N) in winter and in the subtropical region (south of 35°N) in summer, associated with the major troughs over East Asia and North America and the weak European trough in winter, and with the relatively steady subtropical high system in summer. A high value center of Ius is at 35°N in spring and 50°N in summer, which might be caused by the seasonal variation of stationary-wave intensity, particularly in association with the interannual variability of trough ridge positions of stationary waves on the monthly mean maps. (2) There exists obvious asymmetry in Ilus, with the steady zones always located in the areas controlled by strong troughs/ridges and the unsteady ones in the areas where the stationary-wave intensity is low. The Ilus in the subtropics (south of 35°N) is larger in winter than in summer, and vice versa in the midlatitude region (north of 35°N). The summertime distribution of Ilus on the whole shows a rather complicated structure. However, North Europe is the most unsteady area for local stationary waves, as represented by high values of Ilus in both summer and winter, while over the North American continent (about 120°E-60°W), the °Ilus is slightly less than 1 in summer, indicating that the stationary waves in this region are more steady than those over other mid and high latitude regions. (3) From North China to Northwest Pacific, there is a high value zone of Ilus in summer, with its center (45°N, 130°E) located in the east of Heilongjiang Province. This influences the summer climate of northern China, including Northeast, North, and Northwest China. It is obvious that the nonstationarity is an intrinsic attribute of stationary waves, and can be regarded as being of the same importance as the intensity and energy-spectrum structure of stationary waves in the studies of the general circulation system. 相似文献