OLR 低频振荡与西太平洋台风的发生

以影响我国西太平洋台风生成区域平均的OLR演变曲线为基础，对1975—1981年经过30—60天滤波处理的OLR场进行合成分析。结果表明，与西太平洋台风生成有关的系统，主要集中于东半球60°E以东的低纬地区。西太平洋和孟加拉湾南部的赤道地区构成一对低频偶极中心，它们之间有密切的联系。赤道印度洋中部地区是OLR低频振荡的一个重要源区，台风多发、间歇和转换阶段都有明显的特点，对台风的生成和间歇的中期预报有一定的参考意义。特别是夏季形势建立后，在30°N附近副高的东西摆动（有明显的低频变化特征）与ITCZ的变化     

西南地区东部夏季典型旱涝年的OLR特征

利用1959—2006年西南地区东部20个测站的逐日降水量资料和1979—2006年全球OLR（Outgoing Longwave Radiation）逐日格点资料, 分析了西南地区东部夏季典型旱涝年OLR的异常特征。结果表明： 按照区域降水指数可确定3个典型干旱年（2006, 1994和1997年）和3个典型洪涝年（1998, 1980和1993年）, 而1998年和2006年分别是1959年以来西南地区东部降水偏多和偏少最明显的年份。西南地区东部典型旱涝年夏季OLR分布有明显的差异, 洪涝（干旱）年, 从青藏高原东部一直到江淮地区OLR值偏低（高）, 同时孟加拉湾南部及赤道东印度洋地区OLR值也偏低（高）, 而菲律宾及其附近地区OLR值偏高（低）。从3个关键区平均的逐日变化来看, 赤道东印度洋地区对流活动典型涝年强于典型旱年, 菲律宾及其附近地区对流活动则是旱年强于涝年, 青藏高原东部至江淮流域地区（包括西南地区东部）极端涝年盛行上升运动。涝年热带地区的ITCZ以向西移动的特征为主, 而旱年热带地区的ITCZ夏季前期则以向东移动的特征为主。典型涝年孟加拉湾南部及赤道东印度洋地区的对流北传的特征较明显, 6月中旬以后大部分时间可以传到30°N以北, 典型旱年孟加拉湾南部及赤道东印度洋地区的对流主要呈现南北振荡、 偶有中断的活动特征, 很少时间能达到30°N。低纬热带地区关键区域OLR 5～9月一般都具有准40天左右的显著低频变化周期, 而准12～15天的准双周变化周期在部分时段也显著。典型涝年夏季OLR 40天左右低频对流经向和纬向传播在西南地区东部区域得到加强, 低频对流偏强, 引起降水偏多, 而典型旱年夏季则相反, OLR 40天左右低频对流经向和纬向传播在该区域得到削弱, 低频对流偏弱, 引起降水偏少。     

东北地区旱涝的OLR特征分析

该文选取了东北地区4个典型多雨年和4个典型少雨年, 利用OLR资料对该地区旱涝年OLR场的时空分布规律及其低频振荡的传播特征进行了合成对比分析.结果表明, 东北旱涝与低纬OLR的分布及其变化密切相关, 特别是西北太平洋副热带高压、西太平洋ITCZ和印度ITCZ的位置和强度以及赤道中东太平洋OLR的距平在旱涝年均有显著差别, 并且热带和副热带OLR低频振荡的向北传播对东北地区夏季降水也有至关重要的影响.     

热带和中高纬地区季节内振荡的特征及其动力学诊断

使用5年低阶全球谱模式资料,对中高纬大气和热带大气季节内振荡的动力学性质和传播特征进行了诊断研究。分析发现模式再现了大气中季节内振荡在热带和中高纬地区的传播特性以及它们之间的差异。热带大气30—60天振荡在速度势场上表现为纬向—波结构和行波特性,而在散度风场上反映了赤道西太平洋—印度洋东西向偶极子型的振荡。中高纬大气30—60天振荡表现为定常波位相和振幅的变化,即波包络的传播特征。它与中高纬地区遥相关型的转换有关,通过遥相关位相和振幅的变化,不仅完成了热带和中高纬地区之间以及热带不同区域之间的能量输送,而且通过这种能量输送过程把南、北半球中高纬地区季节内振荡联系起来。      

印度洋偶极子对热带大气季节内振荡传播的可能影响

利用多种大气和海温资料,通过相关、合成分析以及个例对比分析,重点研究了热带印度洋偶极型海温模态对热带大气季节内振荡传播的可能影响。结果表明:东南印度洋30～60天OLR距平及赤道印度洋中部30～60天850 hPa纬向风距平都与偶极子指数显著相关;印度洋正（负）偶极型海温模态对应的东印度洋异常冷（暖）水以及赤道印度洋中部850 hPa东（西）风距平阻碍（促进）了季节内对流活动的持续性东传,使得MJO的传播在赤道东印度洋-西太平洋发生明显的中断（持续）。      

30—60天大气振荡的全球特征

利用ECMWF格点资料,分析研究了大气季节内(30—60天)振荡的全球特征。30—60天振荡动能的分布表明高纬度地区要比赤道地区大得多。说明那里有较突出的30—60天振荡。中高纬度地区的30—60天振荡与热带有明显不同,垂直结构为正压模态,以纬向2—4波为主,多为向酉传播。30—60天振荡存在明显的低频遥相关,北半球主要为欧亚—太平洋(EAP)型和PNA型,南半球主要有澳洲—南非(ASA)型和环南美(RSA)型,并且在全球范围构成南北半球相互衔接的低频波列,即EAP-ASA波列和PNA-RSA波列。南北半球30—60天大气振荡有明显的相互影响,本文研究了南北半球30—60天振荡相互影响的3种主要过程。     

热带低层大气30～60天低频动能的年际变化与ENSO循环

利用NCEP再分析资料,通过统计相关及合成分析研究了热带大气季节内振荡(ISO)的年际变化与ENSO循环之间的关系.结果表明,热带大气季节内振荡(也称30～60天低频振荡)的年际变化在热带中西太平洋地区最强.在ElNino成熟之前的春夏季,热带西太平洋的30～60天振荡异常活跃,其动能明显增加且逐渐东移;在E1Nino成熟以后,热带西太平洋大气30～60天低频振荡迅速减弱.与这种加强的30～60天振荡相伴随,在赤道北侧为异常的气旋式环流,赤道地区出现偏西风异常.相反,在LaNina成熟之前的春夏季,热带西太平洋大气30～60天振荡偏弱.进一步的分析还发现,东亚冬季风的年际变化是引起热带大气30～60天振荡的年际变化的主要机制:强东亚冬季风导致热带西太平洋积云对流加强,从而引起热带西太平洋大气30～60天振荡加强;相反,对应于弱的东亚冬季风,热带西太平洋地区积云对流偏弱,大气30～60天振荡偏弱.作者的资料分析还证实,热带大气30～60天低频振荡的年际变化,作为一种外强迫,对ElNino的形成起着十分重要的作用.     

黄河中下游地区夏季逐候降水量的低频振荡特征

本文使用主分量分析黄河中下游地区(河南省)68站1982—1987年夏季(6—8月)逐侯降水量的主要时空特征,并用非整波技术分析所提取的第一主要分量频谱分布的低频振荡特点.分析结果表明该地区降水主要低频振荡周期为6—12候(30—60天)月际振荡及季问振荡15—24候(75—120天).它们年际变化有准两年振荡,其中月际低频振荡与赤道地区的纬向风准两年周期振荡有同相关系.     

南海—热带西北太平洋地区季节内尺度海气变化关系

本文系统地回顾了作者近年来关于南海-热带西北太平洋地区大气和海洋季节内尺度变化关系方面的主要研究成果。文中对10~20天和30~60天两种季节内振荡海气变化关系的不同以及冬、夏季间的差异进行了系统地比较。相比较而言,大气中10~20天振荡所占比例大于30~60天振荡,海表温度30~60天的振荡在南海和西北太平洋副热带地区比10~20天振荡的贡献大,而在低纬度西太平洋地区10~20天振荡与30~60天振荡贡献相近或稍大。在北半球夏季,10~20天低频振荡的分布呈西南—东北走向,由赤道西太平洋地区向西北偏西方向传播,而30~60天低频振荡则以东西向分布为主,表现为由南向北的传播特征。在北半球冬季,10~20天和30~60天两种低频振荡的水平结构类似,均表现为西南—东北走向;同时,南海地区季节内变化信号表现出明显的向南传播的独特特征,并与东亚冬季风的季节内变化密切相关。北半球夏季,南海—菲律宾海地区10~20天低频振荡强度在厄尔尼诺发展年得到加强,而30~60天低频振荡强度则在拉尼娜衰减年得以加强。分析还指出,热带西北太平洋地区夏季热带辐合带附近的季节内变化,尤其是10~20天尺度变化,对季节平均海表温度异常有显著的反馈作用。     

1983与1985年夏季北半球500hPa高度场大气低频波振特征

本文利用观测资料分析了１９８３年１９８５年夏半半球５００ｈＰａ高度场大气低频波的振荡特征。结果表明，１９８３年（厄尔尼诺年）夏季热带中、东太平洋和印度洋以及东亚季风区上空的低频振荡比１９８５年（反厄尔尼诺年）夏季的低频振荡强，而热带西太平洋的情况恰好相反。这是由于反厄尔尼诺年夏季热带西太平洋对流活动强盛所致。分析结果还表明：１９８３年夏季低频波基本上是东传的；１９８５年夏季，在中高纬度地区低频波主     

Interactions between the 30–60 day oscillation,the walker circulation and the convective activities in the tropical western pacific and their relations to the interannual oscillation

In this paper, interactions between the 30-60 day oscillation, the Walker circulation and the convective activities in the tropical western Pacific during the Northern Hemisphere summer are analyzed by using the observed data of wind fields and high-cloud amounts for the period from 1980 to 1989.The analyzed results show that the 30-60 day oscillation (hereafter called LFO) may be largely affected by the convective activities in the tropical western Pacific. The LFO in the tropical western Pacific during the strong convective activities around the Philippines stronger than those during the weak convective activities around the Philippines. Moreover, in the case of strong convective activities around the Philippines, the LFO in the tropical west-ern Pacific and tropical eastern Indian Ocean generally propagates westward, and it is intensified by the LFO with a westward propagating center of maximum oscillation from the east to 140oE. However, in the case of weak convective activities around the Philippines, the LFO gradually becomes stronger with a eastward propagating center of maximum oscillation from the eastern Indian Ocean to the tropical western Pacific.Corresponding to the 30-60 day oscillation, the Walker circulation is also in oscillation over the tropical Pacific and its circulation cell seems to shift gradually westward from the tropical western Pacific to the tropical eastern In-dian Ocean with strong convective activities around the Philippines. This may maintain the intensification of convective activities there. However, during the weak convective activities around the Philippines, the Walker circula-tion gradually moves eastward and an ascending flow may appear in the equatorial central Pacific. This may cause convective activities to be intensified over the equatorial central Pacific.The analyzed results also show that the LFO in the tropical western Pacific and East Asia may be associated with the interannual oscillation of the SST anomaly in the tropical western Pacific.     

POSSIBLE INFLUENCES OF THE TROPICAL INDIAN OCEAN DIPOLE ON THE EASTWARD PROPAGATION OF MJO

Based on multiple datasets, correlation and composite analyses, and case studies, this paper investigated possible influences of the Indian Ocean dipole （IOD） mode on the eastward propagation of intraseasonal oscillation in the tropical atmosphere. The results showed that （1） the 30-60 day outgoing longwave radiation anomalies in the southeastern Indian Ocean and the 30-60 day 850-hPa zonal wind anomalies over the equatorial central Indian Ocean were significantly correlated with the IOD index; （2） during positive IOD years, the anomalously cold water in the southeastern Indian Ocean and the 850-hPa anomalous easterlies over the equatorial central Indian Ocean might act as barriers to the continuously eastward propagation of the intraseasonal convection, which interrupts the Madden-Julian oscillation （MJO） propagation in the eastern equatorial Indian Ocean and western Pacific; and （3） during negative IOD years, the anomalously warm water in the southeastern Indian Ocean and the low-level westerly anomalies over the equatorial central Indian Ocean favor the eastward movement of MJO.     

OLR与长江中游夏季降水的关联

用SVD方法分析了1、4、7月全球OLR与夏季(6—8月)中国华中区域降水场的关系,结果表明:若1月南非东部沿岸至西印度洋、北美北部OLR(Outgoing Longwave Radiation)偏低(偏高),或北非、美国西南沿岸及近海OLR偏高(偏低),则夏季长江中游降水将偏多(偏少)。若4月澳大利亚至东印度洋、日界线以东热带太平洋OLR偏低(偏高),或西北太平洋偏高(偏低),则夏季长江中游降水将偏多(偏少)。若7月东印度洋—澳大利亚大陆、东亚OLR偏低(偏高),则夏季华中区域长江及其以北降水将偏多(偏少),湖南和江西南部降水将偏少(偏多)。夏季长江中游旱、涝年前期OLR明显的区别在于热带太平洋:涝年1月东、西太平洋为明显负、正异常,4月这种异常进一步加剧;旱年1月正好相反,东、西太平洋为微弱的正、负异常,4月转为东、西太平洋为微弱的负、正异常。太平洋暖池OLR低值区(强对流区)4、7月持续偏南,是夏季长江中游降水偏多的另一重要信号。冬、春季OLR与夏季长江中游降水大尺度关联的可能机制为:若1月热带东、西太平洋OLR为明显负、正异常,4月这种异常进一步加剧,也即冬、春季热带太平洋Walker环流持续减弱,从而使夏季暖池对流活动减弱,热带辐合带偏南,Hadley环流偏弱,使夏季西太平洋副热带高压主体位置偏南,导致中国夏季主雨带不能北推至黄河流域,而长期滞留长江中下游,最后造成长江中游降水异常。     

Global-scale intraseasonal and annual variation of divergent water-vapor flux

Summary The global-scale intraseasonal and annual variations of divergent water-vapor transport and water vapor itself were examined by using outgoing longwave radiation (OLR) and data for 1979–1986 produced by the Global Data Assimilation System of the National Meteorological Center. An effort was also made to contrast results of this study with previous analyses of OLR and upper-level divergent circulation.As for intraseasonal oscillation, positive (negative) precipitable-water (W) anomalies and negative (positive) OLR couple with the convergent (divergent) center of the potential function of water vapor transport () anomalies and the divergent (convergent) center of upper-level divergent-circulation anomalies. It is inferred that the eastward-propagating divergent circulation of intraseasonal oscillation converges water vapor to maintain cumulus convection, which releases latent heat, possibly to support this low-frequency oscillation. Fluctuations of W and cumulus convection associated with this oscillation are large over the equatorial Indian Ocean and the equatorial western Pacific, but small over the tropical Americas and equatorial Africa. Moreover, during northern summer, W anomaly bands migrate regularly northward, following the low-level transient 30–50 day monsoon troughs and ridges over the northern Indian Ocean. To the south of the equator, a regular southward propagation of W anomaly bands is identified in both northern summer and winter. In contrast; over the northwestern Pacific, a signature depicting the north-south intraseasonal oscillation of the north Pacific Convergence Zone can be inferred by W anomalies.The annual cycle components of W and cumulus convection inferred from OLR anomalies exhibit three pairs of maximum-minimum centers over tropical continents. These centers correspond to those of and upper-level divergent circulation anomalies. It is shown that landmass cooling in the winter hemisphere and landmass warming in the summer hemisphere establish a pair of upper-level convergent-divergent centers over each tropical continent. Water vapor is converged (diverged) by divergent circulation, in order to maintain maximum (minimum) centers of W and cumulusconvection anomalies over each tropical continent.With 7 Figures     

冬夏季节热带副热带OLR场的遥相关分析

本文利用NOAA13年月平均格点资料分析了冬夏热带副热带射出长波辐射(OLR)的气候特征及其遥相关结构。结果表明,OLR场的高低值带有明显的季节变动,低值带中心从冬至夏由赤道西太平洋地区向西北移至孟加拉湾,高值带从冬至夏北移约10—15个纬度,但东南太平洋高值区的位置无明显季节变动。 遥相关结构分析表明,冬夏季节OLR场分别有8个遥相关关键区,它们之间存在着较强的同时性遥相关联系。冬季遥相关型主要由位于赤道低纬度“印度洋—西太平洋—东太平洋—大西洋”的纬向2波式遥相关和在太平洋中部、东亚地区,南北半球副热带与赤道地区的经向负遥相关型组成。夏季OLR遥相关关键区主要分布在孟加拉湾至赤道西太平洋、东太平洋与低纬度大西洋和中纬度东亚沿海与北美大陆,构成低纬度和中纬度两类纬向正遥相关型。进一步分析发现,冬夏OLR遥相关型的年际变化较好地揭示了OLR场异常与ENSO、低纬度Walker、Hadley环流等海—气系统异常的整体联系。      

热带季节内振荡时空特征的诊断研究

文中应用谱分析、小波分析等方法及较长时段的资料进一步总结了热带季节内振荡的一些基本气候特征。热带季节内振荡主要活跃在 3个地区 ,最强的是西太平洋地区 ,其次是印度洋地区 ,第三是东太平洋沿岸的赤道以北地区。热带季节内振荡有明显的季节变化 ,西太平洋地区和印度洋地区的季节内振荡 1a中有两次极大值 ,冬季主要活跃在南半球 (10°S附近 ) ,而夏季则活跃在北半球 (10°N附近 ) ,春、秋季热带季节内振荡则明显减弱。东赤道太平洋北侧的季节内振荡只在夏季活跃 ,而冬季则很弱 ,且不随季节而南北移动。对于大气的大尺度要素 ,例如u风场 ,热带季节内振荡的能量主要集中在 1波。而对于像降水这样尺度较小的要素 ,热带季节内振荡的能量则相对较分散 ,尽管它仍然在 1波有最大的能量 ,但 2～ 4波也具有较接近的能量。热带季节内振荡以东移的波动为主。热带季节内振荡存在着年际甚至更长时间的变化。 2 0世纪 70年代末期季节内振荡的幅度有一明显的突变。     

WESTWARD PROPAGATING LOW-FREQUENCY OSCILLATION AND ITS TELECONNECTION IN THE EASTERN HEMISPHERE

By use of daily OLR data of eight years (1975—1977,1979—1983),the propagation features of 30—60day low-frequency oscillation (LFO) and its teleconnections are studied.The results are as follows:(1)The LFO is quite active in the regions of the South China Sea,mainland of China and subtrop-ical western-North-Pacific.(2)The zonal propagation direction of LFO is eastward along the equator and gradually changes towestward north of 10°N and south of 10°S.The westward propagation of LFO dominates in the areaof 15°N-30°N,Eastern Hemisphere.(3)In the region of east Asia (120°E),the main meridional directions are northward in tropics andsouthward in high latitudes.These two opposite propagating LFO are merged in the vicinity of subtropics.Sometimes,the northward propagating LFO can penetrate through the subtropics to high latitudes and viceversa.On the average,the northward propagation dominates in summer time.(4)The EOF analysis of the summer data shows that there are two main eiginvector centers of OLR-LFO,one is located over the Bay of Bengal and the other over the tropical western-North-Pacific.Thesign of these two centers are just opposite to each other.It should be noted that on the normal,thesetwo oscillation centers mentioned above coincide with the two strong centers of atmospheric 12eat source insummer.It means that the activities of LFO in the Indian monsoon system and the East Asian monsoonsystem are reverse.For the first component of eiginvector,a belt of LFO with the same sign stretcheswith a SW-NE direction from the tropical center in the western-North-Pacific northwestward,passing bythe point at 15°N,180°E and reaches southwestern states of the United States.To the north and southof this belt,there are other two belts with opposite sign.Again further north and south of them,there areother two belts with the same sign as the first one.Furthermore,to the NW (near Taiwan) and SE (10°S,160°W) of the tropical East Asian center,there is,respectively,another center with opposite sign.Analmost straight line can go through all three centers.The main characteristics of the second,third andfourth components of eiginvector are the same as that of the first one.It indicates that the teleconnectioncentered around the tropical East Asian center of LFO is characterized by a SW-NE oriented wave frontand the energy transport of oscillation from SE to NW.That is to say,the oscillations in the tropicalwestern-North-Pacific may be the source of those in China during summer.We call this teleconnection pat-tern the WPC (western Pacific-China) pattern so as to distinguish from the PNA pattern.     

东亚梅雨季节内振荡的气候特征

影响中国、日本、朝鲜半岛的东亚梅雨是夏季风向北推进过程中的特有雨季。利用NCEP/NCAR逐日再分析资料、CMAP降水资料,将夏季风影响及夏季风降水的季节转换相结合,定义东亚梅雨的入、出梅指标;进而采用集合经验模态分解信号提取方法对东亚梅雨区降水季节内振荡及其大尺度环流条件的气候特征进行了详细分析;并对东亚梅雨季节内振荡对降水事件的指示作用进行讨论,为东亚梅雨区降水的延伸预报提供依据和参考。研究结果表明:(1)采用标准化候降水量的空间覆盖率,同时兼顾夏季风影响等条件确定的东亚梅雨入、出梅划分指标可较好地反映东亚梅雨的气候特征及东亚梅雨期的大尺度环流形势。(2)东亚梅雨全年降水量存在三峰型分布特征,峰值分别位于第27、36及47候。该三峰型特征主要受10—20及30—60d的低频振荡影响。比较而言,30—60d振荡对梅雨区降水三峰型的贡献较10—20d振荡大。(3)东亚梅雨区峰值降水与热带环流及北方高位涡冷空气输送的低频演变密切关联。在梅雨区北侧,中高纬度里海附近冷空气(高位涡)低频波列的东传及鄂霍次克海高位涡的西南向输送共同影响东亚梅雨区。在梅雨区南侧,通过热带低频异常强对流的激发作用,热带西太平洋至中国东北—鄂霍次克海地区形成沿经向分布的低层气旋-反气旋-气旋-反气旋波列,进而导致梅雨区低层形成低频偏北风和偏南风的辐合;而印度西海岸和阿拉伯海地区异常对流活动产生的波列向东北方向传播,亦对梅雨区低频峰值降水产生影响。对于低频谷值降水的大气低频演变,情况与上述基本相反。(4)东亚梅雨区降水不同位相下出现极端降水事件的概率有明显差异。梅雨区降水低频峰(谷)值位相下出现异常多(少)降水量的概率约为30%。因此,上述梅雨区降水低频振荡演变相关的大气低频振荡特征对梅雨区降水事件的延伸预报具有参考价值。     

Comparison of the Structure and Evolution of Intraseasonal Oscillations Before and After Onset of the Asian Summer Monsoon

High-resolution satellite-derived data and NCEP-NCAR reanalysis data are used to investigate intraseasonal oscillations （ISO） over the tropical Indian Ocean.A composite evolution of the ISO life cycle is constructed,including the initiation,development,and propagation of rainfall anomalies over the tropical Indian Ocean.The characteristics of ISO over the tropical Indian Ocean are profoundly different before and after the onset of the Indian summer monsoon.Positive precipitation anomalies before monsoon onset appear one phase earlier than those after monsoon onset.Before monsoon onset,precipitation anomalies associated with ISO first initiate in the western tropical Indian Ocean and then propagate eastward along the equator.After monsoon onset,convective anomalies propagate northward over the Indian summer monsoon region after an initial eastward propagation over the equatorial Indian Ocean.Surface wind convergence and air-sea interaction play critical roles in initiating each new cycle of ISO convection.