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1.
副热带急流强度和赤道QBO对平流层突然增温的影响   总被引:2,自引:0,他引:2       下载免费PDF全文
使用一个全球原始方程半谱模式模拟了副热带急流强度和赤道准两年振荡(QBO)对平流层突然增温(SSW)的影响.结果指出:副热带急流强度对SSW有明显影响,副热带急流越强,SSW发展越快,极区最大增温区的高度越低;赤道QBO不同相位零风线的南北位移对SSW没有明显影响;QBO东风相位时副热带急流更强,而QBO西风相位时副热带急流较弱的观测事实,可能是大的中冬SSW更容易发生在QBO东风相位的主要原因.  相似文献   

2.
建立了一个反映厄尔尼诺/南方涛动(ENSO)与热带远西太平洋准两年振荡(QBOWP)相互作用最基本物理过程的新概念模式. 在此概念模式中, QBOWP对ENSO的影响通过两种途径: (1) 沿赤道太平洋海洋Kelvin波和 (2) 大气的Walker环流; 而ENSO对QBOWP的影响则可通过大气的Walker环流异常来实现. 对该模式结果的分析诊断表明: 在ENSO与QBOWP相互作用过程中, 大气桥(Walker环流)的作用比海洋桥(沿赤道太平洋的Kelvin波)更重要; 通过QBOWP与ENSO的相互作用, 一个3~5年周期的ENSO振荡可以变为准两年振荡, 而赤道远西太平洋年际变化的主要周期也会变长; 热带太平洋大气-海洋耦合系统的多时间尺度的年际变化可以通过ENSO与QBOWP的相互作用来实现.  相似文献   

3.
热带太平洋海洋混合层水体振荡与ENSO循环   总被引:3,自引:0,他引:3  
研究了热带太平洋温跃层和海面风应力年际变率主要模态及它们之间的相互作用, 探讨了ENSO循环的可能形成机制, 得到如下结果: (1)热带太平洋温跃层异常具以160°W为纵轴的东西向偶极子分布和以6~8°N为横轴的南北向跷跷板分布等两种主要模态, 两者(相位差90°)组合构成El Niño/La Niña循环, 表现为混合层水体(指温跃层界面之上海温垂直分布较均匀的上层海洋)在赤道与12°N之间的热带太平洋海盆内反时针三维振荡; (2)热带太平洋风应力异常具两种主要分布型, 第一特征向量场反映了热带太平洋信风异常导致的赤道太平洋异常纬向风应力及散度场与离赤道北太平洋异常越赤道风应力及反相散度场, 第二特征向量场反映了热带辐合带(ITCZ)异常导致的异常风应力及相应散度场; (3)信风异常对ENSO事件的形成、强度和相变都有决定性的作用, 它导致海面倾斜, 提供了混合层水体振荡初始位能, 同时造成赤道太平洋西部与东部之间和赤道太平洋与12°N北太平洋海盆之间温跃层同步反相位移, 限定了热带太平洋混合层水体振荡的振幅和路线. ITCZ异常主要对ENSO相变过程有一定影响; (4)热带西太平洋海洋热力异常导致海面风应力异常, 它伴随热带太平洋混合层水体振荡沿赤道由西向东扩展, 造成热带太平洋信风异常, 产生有利于水体振荡的异常风应力及散度场, 反过来进一步加强混合层水体振荡. 这一海气耦合过程与混合层水体振荡一起为ENSO循环提供了相变和年际记忆机制. 研究指出, ENSO循环实质上是由信风异常和海气耦合过程共同作用下产生的热带太平洋海洋混合层水体在赤道与12°N之间热带太平洋海盆内的惯性振荡. 海气耦合过程产生的作用力大于或等于水体运动阻力时, ENSO循环将加强或维持, 不足以克服水体运动阻力时, 水体振荡减小, ENSO循环将逐渐减弱, 直至中断.  相似文献   

4.
赤道MJO活动对南海夏季风爆发的影响   总被引:6,自引:0,他引:6       下载免费PDF全文
利用1979—2013年NCEP/DOE再分析资料的大气多要素日平均资料、美国NOAA日平均向外长波辐射资料和ERSST月平均海温资料,分析赤道大气季节内振荡(简称MJO)活动对南海夏季风爆发的影响及其与热带海温信号等的协同作用.结果表明,赤道MJO活动与南海夏季风爆发密切联系,MJO的湿位相(即对流活跃位相)处于西太平洋位相时,有利于南海夏季风爆发,而MJO湿位相处于印度洋位相时,则不利于南海夏季风爆发.赤道MJO活动影响南海夏季风爆发的物理过程主要是大气对热源响应的结果,当MJO湿位相处于西太平洋位相时,一方面热带西太平洋对流加强使潜热释放增加,导致处于热源西北侧的南海—西北太平洋地区对流层低层由于Rossby响应产生气旋性环流异常,气旋性环流异常则有利于西太平洋副热带高压的东退,另一方面菲律宾附近热源促进对流层高层南亚高压在中南半岛和南海北部的建立,使南海地区高层为偏东风,从而有利于南海夏季风建立;当湿位相MJO处于印度洋位相时,热带西太平洋对流减弱转为大气冷源,情况基本相反,不利于南海夏季风建立.MJO活动、孟加拉湾气旋性环流与年际尺度海温变化协同作用,共同对南海夏季风爆发迟早产生影响,近35年南海夏季风爆发时间与海温信号不一致的年份,基本上是由于季节转换期间的MJO活动特征及孟加拉湾气旋性环流是否形成而造成,因此三者综合考虑对于提高季风爆发时间预测水平具有重要意义.  相似文献   

5.
外热带大气扰动对ENSO的影响   总被引:4,自引:0,他引:4       下载免费PDF全文
薛峰  何卷雄 《地球物理学报》2007,50(5):1311-1318
合成分析了20世纪80年代以来5次主要的ENSO事件,发现外热带大气扰动通过经向风异常不仅对ENSO的发生起到重要的触发作用,而且影响到ENSO的发展和衰减. 因此,尽管ENSO对外热带大气扰动有影响,但同时外热带大气扰动又与ENSO有相互作用. 在ENSO发生前,南印度洋中纬度为反气旋异常,并通过Rossby波的频散作用加强了澳大利亚附近的反气旋异常;同时,澳大利亚东部沿海的南风异常与菲律宾附近的北风异常在赤道辐合,促进了赤道西太平洋西风异常的爆发和其后ENSO的发生. 在ENSO发生之后,东南太平洋上的气旋异常及相关的南风异常进一步增强了赤道中东太平洋的西风异常和ENSO的发展. 当ENSO达到成熟时,澳大利亚东部的反气旋异常东移,使东南太平洋的气旋异常减弱,南方涛动型环流异常亦随之减弱;同时,阿留申气旋异常加强,尤其是副热带北太平洋的风场异常可加强赤道中东太平洋海水的涌升,使该地区海表温度降低,加速ENSO的消亡.  相似文献   

6.
利用1949~2005年NCEP/NCAR逐日再分析资料及登陆中国的热带气旋资料, 采用功率谱分析、相关分析研究了近57 a夏半年(6~10月)赤道气压低频振荡的变化特征及其与登陆中国热带气旋的关系. 结果表明, 夏半年赤道气压主要表现为5~7, 10~30 d的周期振荡, 赤道气压准双周振荡强度的年际变化与登陆中国热带气旋个数有明显的正相关. 用小波逆变换对近57 a逐年5~11月逐日赤道气压进行准双周振荡滤波, 统计得到近57 a 6~10月与7~9月赤道气压准双周振荡波谷前后4 d内有热带气旋登陆中国沿海地区的几率分别为59.7%, 73.0%. 用合成分析方法建立了7~9月赤道气压准双周振荡波谷附近有、无热带气旋登陆中国的大气环流模型. 当赤道气压准双周振荡波谷附近有(无)热带气旋登陆中国时, 东半球中高纬度盛行纬向(经向)环流, 卾霍次克海附近的高压脊偏弱(偏强),西风带偏北(偏南), 副高偏西(偏东)偏强(偏弱), 东南亚越赤道气流偏强(弱), 西南季风偏强(弱)且在波谷时更强(弱), 有(不)利于热带气旋登陆中国. 所建赤道气压准双周振荡波谷附近有、无热带气旋登陆中国的大气环流模型可以较好地反映两者大气环流场的差异, 有利于做好登陆中国热带气旋的中期预报.  相似文献   

7.
本文分析了夏季西北太平洋大气环流异常特征及其与海温变化的关系,发现夏季西北太平洋异常反气旋/气旋(WNPAC/WNPC)是西北太平洋地区对流层中低层存在的重要大气环流异常现象,与东亚-西北太平洋低纬度至高纬度的经向PJ波列及欧亚中高纬度东西纬向波列的变化有关,通过与中高纬度环流变化的联系,对东亚及欧亚中高纬度气候有重要影响.夏季WNPAC/WNPC与热带海温变化的关系存在明显的不对称性,显著的WNPAC一般出现在El Niño衰减年夏季,与前期El Niño成熟年冬季的赤道东太平洋暖海温异常和El Niño衰减年春夏季印度洋海盆尺度的暖海温异常有明显的正相关关系,进一步表明了WNPAC在El Niño事件影响夏季气候中的重要桥梁作用;而夏季显著的WNPC与前期和同期热带海温变化的关系存在明显的不确定性,主要与夏季热带印度洋和赤道中东太平洋之间东暖西冷的热力差异异常引起的孟加拉湾-赤道西太平洋西风异常有关.进一步分析WNPAC/WNPC与海温变化关系不对称的可能原因,发现El Niño和La Niña衰减年夏季热带印度洋和太平洋海温变化所引起的印-太之间海温(热力)差异的一致性特征可能是导致WNPAC/WNPC与海温变化关系不对称的主要原因.  相似文献   

8.
利用Hadley中心的月平均海温资料、NCEP/NCAR和ERA-Interim逐日再分析大气环流数据等,详细对比了赤道大气季节内振荡(MJO)活动在东部型El Ni?o与中部型El Ni?o发展期间的异同点.结果表明,与传统的东部型El Ni?o发展前MJO明显偏强的特征相似,在中部型El Ni?o迅速发展前的春夏季,MJO动能亦较强且持续东传特征显著.这说明无论是东部型El Ni?o还是中部型El Ni?o,与MJO能量的突然增长相联系的低频纬向西风和低频对流活动的增强及其持续东传是激发El Ni?o的重要因素.但是,在中部型El Ni?o发展成熟的冬季至次年春季,热带中西太平洋MJO动能的强度突然再次增强,所占大气总扰动动能的比重也再次增大,热带MJO动能的逐日演变达到第二次峰值,且较第一次峰值更强;MJO从热带印度洋向赤道中东太平洋持续东传的特征也更为显著.这与在传统东部型El Ni?o盛期MJO能量和东传都明显减弱的特征表现出显著的差异.进一步分析指出,中部型El Ni?o成熟期海温正距平中心位置的西移以及由中部型El Ni?o激发的范围偏小、位置偏西的菲律宾附近异常反气旋环流可能是导致中部型El Ni?o盛期MJO活动显著增强的主要原因.  相似文献   

9.
分析了1985~1988年期间一条从奥斯陆(NORESS)经赫尔辛基至列宁格勒(OHL剖面)的东西向剖面用NORESS台阵记录的147次工业爆破的波形。事件离NORESS台阵的距离为250~1300km,且近震震级在2.0~3.5范围内。由赫尔辛基大学的区域地震台网提供的震源位置和发夺时刻为NORESS台阵走时估计尔辛基大学的区域地震台网提供的震源位置和发震时刻为NORESS台阵走时估计提供了可靠  相似文献   

10.
何翔 《地震》1994,(4):65-72
本文利用永胜台水管倾斜仪观测资料分别进行了资料长度为1月和1年的维尼迪科夫调和分析。研究了振幅因子与地震的关系,发现地震前EW2分量M2波与NS分量O1波的γ值具有不同程序的异常变化,异常量为1.5%-7.7%;在地震发生前或地震发生时,各个主潮波γ值误差变大。用震例分析证明了倾斜固体潮振幅异常用于地震预报的可行性。  相似文献   

11.
李熠  杨修群  谢倩 《地球物理学报》2010,53(7):1543-1553
利用NCEP/NCAR大气再分析资料以及Hadley中心海表温度资料,针对北太平洋副热带高压(简称副高)的完整系统,通过分析超前于ENSO事件的海平面副高年际异常特征及其对ENSO事件的触发作用以及ENSO事件对500 hPa副高和海平面副高的滞后影响,结果表明了北太平洋副热带高压年际变异和ENSO循环之间存在选择性相互作用.即在大多数情况下,一方面,前期海平面副高减弱会导致热带西太平洋表面西风异常,通过海洋平流过程触发El Nino事件在夏季发生发展,在秋冬季成熟; 而另一方面,El Nino事件在秋冬季发展成熟后,增强了赤道中太平洋的对流性热源,通过对异常热源的动力响应,同期和次年夏季500 hPa副高增强,又通过增强的Hadley环流作用,副热带地区下沉运动增强,从而使得次年夏季海平面副高增强,增强的海平面副高又有利于触发下一个La Nina事件.副高年际变异和ENSO循环之间相互作用的选择性主要取决于副高异常是否接近于赤道以及ENSO事件本身的持续性.这种相互作用有利于在热带太平洋海气系统产生准两年振荡.  相似文献   

12.
Mixed-layer water oscillations in tropical Pacific for ENSO cycle   总被引:2,自引:0,他引:2  
The main modes of interannal variabilities of thermocline and sea surface wind stress in the tropical Pacific and their interactions are investigated,which show the following results.(1) The thermocline anomalies in the tropical Pacific have a zonal dipole pattern with 160°W as its axis and a meridional seesaw pattern with 6-8°N as its transverse axis.The meridional oscillation has a phase lag of about 90° to the zonal oscillation,both oscillations get together to form the El Ni?o/La Ni?a cycle,which be-haves as a mixed layer water oscillates anticlockwise within the tropical Pacific basin between equator and 12°N.(2) There are two main patterns of wind stress anomalies in the tropical Pacific,of which the first component caused by trade wind anomaly is characterized by the zonal wind stress anomalies and its corresponding divergences field in the equatorial Pacific,and the abnormal cross-equatorial flow wind stress and its corresponding divergence field,which has a sign opposite to that of the equatorial region,in the off-equator of the tropical North Pacific,and the second component represents the wind stress anomalies and corresponding divergences caused by the ITCZ anomaly.(3) The trade winds anomaly plays a decisive role in the strength and phase transition of the ENSO cycle,which results in the sea level tilting,provides an initial potential energy to the mixed layer water oscillation,and causes the opposite thermocline displacement between the west side and east side of the equator and also between the equator and 12°N of the North Pacific basin,therefore determines the amplitude and route for ENSO cycle.The ITCZ anomaly has some effects on the phase transition.(4) The thermal anomaly of the tropical western Pacific causes the wind stress anomaly and extends eastward along the equator accompanied with the mixed layer water oscillation in the equatorial Pacific,which causes the trade winds anomaly and produces the anomalous wind stress and the corresponding divergence in favor to conduce the oscillation,which in turn intensifies the oscillation.The coupled system of ocean-atmo-sphere interactions and the inertia gravity of the mixed layer water oscillation provide together a phase-switching mechanism and interannual memory for the ENSO cycle.In conclusion,the ENSO cycle essentially is an inertial oscillation of the mixed layer water induced by both the trade winds anomaly and the coupled ocean-atmosphere interaction in the tropical Pacific basin between the equator and 12°N.When the force produced by the coupled ocean-atmosphere interaction is larger than or equal to the resistance caused by the mixed layer water oscillation,the oscillation will be stronger or maintain as it is,while when the force is less than the resistance,the oscillation will be weaker,even break.  相似文献   

13.
Interaction between the Quasi-Biennial Oscillation in far west equatorial Pacific (QBOWP) and the El Nino/Southern Oscillation (ENSO) is studied using a new conceptual model. In this conceptual model, the QBOWP effects on ENSO are achieved through two ways: (1) the oceanic Kelvin wave along equatorial Pacific, and (2) the Atmospheric Walker Circulation anomaly, while ENSO effects on QBOWP can be accomplished by the atmospheric Walker Circulation anomaly. Diagnosis analysis of the model results shows that the Atmospheric bridge (Walker circulation) plays a more important role in interaction between the ENSO and QBOWP than the oceanic bridge (oceanic Kelvin wave along equatorial Pacific); It is found that by the interaction of the ENSO and QBOWP, a free ENSO oscillation with 3-5 years period could be substituted by a oscillation with the quasi-biennial period, and the dominant period of SST anomaly and wind anomaly in the far west equatorial Pacific tends to be prolonged with enhanced ENSO forcing. Generally, the multi-period variability in the coupled Atmosphere-Ocean System in the Tropical Pacific can be achieved through the interaction between ENSO and QBOWP.  相似文献   

14.
南印度洋副热带偶极模在ENSO事件中的作用   总被引:8,自引:0,他引:8       下载免费PDF全文
晏红明  李崇银  周文 《地球物理学报》2009,52(10):2436-2449
南印度洋副热带偶极模(Subtropical Dipole Pattern,SDP)是印度洋存在的另一种很明显的偶极型海温差异现象,在年际和年代际尺度上均有十分明显的表现.而目前有关印度洋海气相互作用的研究主要集中在赤道印度洋地区,针对南印度洋地区的工作还比较少,特别是有关南印度洋海温与ENSO(El NiDo-Southern Oscillation)事件关系的研究.本文初步探讨了年际尺度上南印度洋副热带偶极型海温变化差异与ENSO事件的关系,发现SDP与ENSO事件有密切的联系,SDP事件就像连接正负ENSO位相转换的一个中间环节,SDP事件前后期ENSO的位相刚好完全相反.进一步,本文通过分析SDP事件前后期海温、高低层风、低层辐合辐散、高空云量和辐射等的变化特征研究了南印度洋偶极型海温异常在ENSO事件中的作用,结果表明:SDP在ENSO事件中的作用不仅涉及海气相互作用的正负反馈过程,还与热带和副热带大气环流之间的相互作用有关,特别是与东南印度洋海温变化所引起的异常纬向风由赤道印度洋向赤道太平洋传播的过程等有十分直接的关系;同时,SDP对ENSO事件的影响在很大程度上还依赖于大尺度平均气流随季节的变换.  相似文献   

15.
Two modes of dipole events in tropical Indian Ocean   总被引:1,自引:0,他引:1  
By analyzing the distributions of subsurface temperature and the surface wind stress anomalies in the tropical Pacific and Indian Oceans during the Indian Ocean Dipole (IOD) events, two major modes of the IOD and their formation mechanisms are revealed. (1) The subsurface temperature anomaly (STA) in the tropical Indian Ocean during the IOD events can be described as a “<” -shaped and west-east-oriented dipole pattern; in the east side of the “<” pattern, a notable tongue-like STA extends westward along the equator in the tropical eastern Indian Ocean; while in the west side of the “<” pattern, the STA has opposite sign with two centers (the southern one is stronger than the northern one in intensity) being of rough symmetry about the equator in the tropical mid-western Indian Ocean. (2) The IOD events are composed of two modes, which have similar spatial pattern but different temporal variabilities due to the large scale air-sea interactions within two independent systems. The first mode of the IOD event originates from the air-sea interaction on a scale of the tropical Pacific-Indian Ocean and coexists with ENSO. The second mode originates from the air-sea interaction on a scale of the tropical Indian Ocean and is closely associated with changes in the position and intensity of the Mascarene high pressure. The strong IOD event occurs when the two modes are in phase, and the IOD event weakens or disappears when the two modes are out of phase. Besides, the IOD events are normally strong when either of the two modes is strong. (3) The IOD event is caused by the abnormal wind stress forcing over the tropical Indian Ocean, which results in vertical transports, leading to the upwelling and pileup of seawater. This is the main dynamic processes resulting in the STA. When the anomalous easterly exists over the equatorial Indian Ocean, the cold waters upwell in the tropical eastern Indian Ocean while the warm waters pileup in the tropical western Indian Ocean, hence the thermocline in the tropical Indian Ocean is shallowed in the east and deepened in the west. The off-equator component due to the Coriolis force in the equatorial area causes the upwelling of cold waters and the shallowing of the equatorial India Ocean thermocline. On the other hand, the anomalous anticyclonic circulations and their curl fields located on both sides of the equator, cause the pileup of warm waters in the central area of their curl fields and the deepening of the equatorial Indian Ocean thermocline off the equator. The above three factors lead to the occurrence of positive phase IOD events. When anomalous westerly dominates over the tropical Indian Ocean, the dynamic processes are reversed, and the negative-phase IOD event occurs. Supported by National Natural Science Foundation of China (Grant No. 40776013), National Basic Research Program of China (Grant No. 2006CB403601) and the Knowledge Innovation Project of Chinese Academy of Sciences (Grant No. KZCX-SW-222)  相似文献   

16.
In the tropical Pacific region, El Ni?o/Southern Os- (COADS SST from 1945 to 1993) in the eastern cillation (ENSO) and the Quasi-Biennial Oscillation in (150°W-90°W, 5°S-5°N) and the observed SST far west equatorial Pacific (QBOWP) are two most and zonal wind in the far western equatorial Pacific prominent interannual variation phenomena. The for- (120°-140°E, 0°-10°N) (Fig.1), in the eastern Pa- mer is characterized by coupled SST-wind variability cific the period of S…  相似文献   

17.
Interaction between the Quasi-Biennial Oscillation in far west equatorial Pacific (QBOWP) and the El Ni?o/Southern Oscillation (ENSO) is studied using a new conceptual model. In this conceptual model, the QBOWP effects on ENSO are achieved through two ways: (1) the oceanic Kelvin wave along equatorial Pacific, and (2) the Atmospheric Walker Circulation anomaly, while ENSO effects on QBOWP can be accomplished by the atmospheric Walker Circulation anomaly. Diagnosis analysis of the model results shows that the Atmospheric bridge (Walker circulation) plays a more important role in interaction between the ENSO and QBOWP than the oceanic bridge (oceanic Kelvin wave along equatorial Pacific); It is found that by the interaction of the ENSO and QBOWP, a free ENSO oscillation with 3–5 years period could be substituted by a oscillation with the quasi-biennial period, and the dominant period of SST anomaly and wind anomaly in the far west equatorial Pacific tends to be prolonged with enhanced ENSO forcing. Generally, the multi-period variability in the coupled Atmosphere-Ocean System in the Tropical Pacific can be achieved through the interaction between ENSO and QBOWP.  相似文献   

18.
Ocean–atmosphere modes of climate variability in the Pacific and Indian oceans, as well as monsoons, regulate the regional wet and dry episodes in tropical regions. However, how those modes of climate variability, and their interactions, lead to spatial differences in drought patterns over tropical Asia at seasonal to interannual time scales remains unclear. This study aims to analyse the hydroclimate processes for both short- and long-term spatial drought patterns (3-, 6, 12- and 24-months) over Peninsular Malaysia using the Standardized Precipitation Index, Standardized Precipitation Evapotranspiration Index, and Palmer Drought Severity Index. Besides that, a generalized least squares regression is used to explore underlying circulation mechanisms of these spatio-temporal drought patterns. The tested drought indices indicate a tendency towards wetter conditions over Peninsular Malaysia. Based on principal component analysis, distinct spatio-temporal drought patterns are revealed, suggesting North–South and East–West gradients in drought distribution. The Pacific El Nino Southern Oscillation (ENSO), the South Western Indian Ocean (SWIO) variability, and the quasi-biennial oscillation (QBO) are significant contributors to the observed spatio-temporal variability in drought. Both the ENSO and the SWIO modulate the North–South gradient in drought conditions over Peninsular Malaysia, while the QBO contributes more to the East–West gradient. Through modulating regional moisture fluxes, the warm phases of the ENSO and the SWIO, and the western phases of the QBO weaken the southwest and northeast monsoon, leading to precipitation deficits and droughts over Peninsular Malaysia. The East–West or North–South gradients in droughts are related to the middle mountains blocking southwest and northeast moisture fluxes towards Peninsular Malaysia. In addition, the ENSO and QBO variations are significantly leading to short-term droughts (less than a year), while the SWIO is significantly associated with longer-duration droughts (2 years or more). Overall, this work demonstrates how spatio-temporal drought patterns in tropical regions are related to monsoons and moisture transports affected by the oscillations over the Pacific and Indian oceans, which is important for national water risk management.  相似文献   

19.
本文根据季节转换前后副高脊面附近经向温度梯度变号的本质,利用相关分析和合成分析等方法研究了季节转换年际变化与外部影响因子的联系. 结果表明,冬春季青藏高原热状况和ENSO(El Nio/Southern Oscillation,厄尔尼诺/南方涛动)是决定亚洲季风区季节转换年际变化的主要因素. 当冬、春季海温呈现El Nio异常时,Walker环流减弱,于是西太平洋暖池区对流活动受到抑制,而赤道东太平洋对流活动加强则强迫赤道印度洋地区产生绝热下沉运动,使得印度洋地区大气偏暖,结果增大了南北向温度梯度,季节转换往往偏晚. 反之,季节转换偏早. 初春高原上空对流层中高层的气温异常对于判断季节转换迟早有很好的指示意义.  相似文献   

20.
给定1948~1999年逐月变化的全球观测的海表温度分布,使用全球大气环流模式(CCM3/NCAR)模拟了大气对海表温度变化的响应,利用SVD和合成检验方法,分析了El Nino发展阶段夏季、成熟阶段冬季以及衰亡阶段夏季东亚大气环流的年际异常型.结果表明:El Nino发展阶段夏季,中国东北、朝鲜半岛以及日本海附近为高度负异常中心,西太平洋副高偏弱、偏东,东亚夏季风增强;El Nino成熟阶段冬季,东亚大槽加强,东亚北部冬季风加强;El Nino衰亡阶段夏季,西太平洋副高偏强、偏南、西伸,东亚夏季风减弱;El Nino事件在其衰亡阶段夏季与东亚大气环流异常的关系最紧密,其次是成熟阶段冬季,最后是发展阶段夏季.模拟的El Nino演变不同阶段东亚大气环流年际异常型易于解释以往研究中观测分析揭示的由El Nino造成的我国东部气温和降水异常型.  相似文献   

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