第四纪两类千年尺度气候振荡现象及机理研究

千年尺度气候突变事件是第四纪冰期普遍存在的气候现象。这些事件可以被分为两类,一类为Dansgaard-Oeschger Event (DO事件),另一类为海因里希(Heinrich Stadial,HS)事件,后者有时也被认为是一种特殊的DO事件,因此也被称为 HS-DO事件。HS事件期间北大西洋冰架的融化一般对应DO振荡的冷相位,这与通常认为的冰架在较冷气候下体积增加并不相符。这两类事件在北大西洋重建数据中表现得最为明显,但其气候影响具有全球性。由于没有显著的外强迫驱动这两类气候突变事件,自20世纪90年代首次被确认以来,HS-DO事件一直是古气候界关注的重点,且人们对其触发机理仍没有定论。本文基于目前对这两类千年事件的研究现状,集中总结了目前已有的可反映千年事件的重建数据,利用已有的模拟工作,重点回顾了现有的机制理论,评述了目前研究DO事件以及HS-DO事件的局限性,并对其后续工作,尤其是模拟部分,进行了展望。     

Resonance of baroclinic waves in the tropical oceans: The Indian Ocean and the far western Pacific

The Indian Ocean has a particularity, its width is close to half the wavelength of a Rossby wave of biannual frequency, this coincidence having been capitalized on by several authors to give the observations a physical basis. The purpose of this article is to show that this is not the case since the resonance of tropical baroclinic waves occurs in all three oceans. This is because the westward-propagating Rossby wave is retroflexed at the western boundary to form off-equatorial Rossby waves dragged by countercurrents before receding and turning back as a Kelvin wave. Thus a quasi-stationary baroclinic wave is formed, whose mean period is tuned to the forcing period. Two independent basin modes resonantly forced are highlighted – 1) a nearly symmetric zonal 1/2-yr period Quasi-Stationary Wave (QSW) that is resonantly forced by the biannual monsoon. It is formed from first baroclinic mode equatorial-trapped Rossby and Kelvin waves and off-equatorial Rossby waves at the western antinode. This QSW controls the Equatorial Counter Current at the node. The Indian Ocean Dipole (IOD) results from a subharmonic mode locking resulting from the coupling of this QSW and the 2nd, 3rd and 4th baroclinic modes - 2) a 1-yr period QSW formed from an off-equatorial baroclinic Rossby wave, which is induced from the southernmost current of the Indonesian Throughflow through the Timor passage, propagating in the southern and northern hemispheres: the drivers are south-easterlies in the southern hemisphere and monsoon wind in the northern hemisphere.     

中高纬环流因子与黑龙江省初夏气候异常分析

利用1954-2010年地面气温、降水观测资料和月环流特征量、NCEP高度场再分析资料等,采用常规气候统计方法,分析了黑龙江省初夏6月气温、降水的气候特点,通过初夏6月气温、降水与北半球500 hPa高度场相关分析,建立起与中高纬度环流因子关系。结果表明：黑龙江省初夏气候异常与中高纬度环流异常有关,影响初夏气候异常的中高纬度环流因子主要有亚洲纬向环流指数,阿留申低压指数,亚洲区极涡面积指数,鄂霍次克海的阻塞高压指数等。在此基础上分析大气及中高纬度环流因子的背景,考虑外强迫因子海温的间接作用,掌握中高纬度环流因子的变化,是准确预测黑龙江省初夏气候的关键前提所在。     

大气季节内振荡对夏季登陆广东台风的影响

基于热带气旋最佳路径资料和向外长波辐射数据,结合高斯滤波、经验正交函数分解和合成分析等方法,探讨了20~90 d周期的MJO(Madden-Julian Oscillation)和10~20 d周期的QBWO(Quasi-Biweekly Oscillation)两类大气季节内振荡对夏季(5-9月)登陆广东台风的影响。结果表明:MJO和QBWO对登陆广东台风个数、强度、位置和运动方向均有显著影响:当MJO和QBWO的对流中心(抑制中心)靠近广东沿岸时,登陆广东的台风数量多(少)、强度大(小)、登陆位置偏东(西)、登陆后东向运动的台风数量偏多(少)。在此基础上,还进一步探讨了MJO和QBWO对生成于南海和西北太平洋的这两类登陆广东台风的影响及两者对登陆广东台风的共同影响。     

1979—2016年四川盆地低涡的气候特征分析

利用6 h一次、水平分辨率为0.25°×0.25°的ERA-Interim再分析资料,对1979—2016年生成于四川盆地的西南涡的发生和发展进行统计分析。结果表明：四川盆地低涡集中生成于盆地内;在6月生成最多,7月发展最强;按移动情况不同可将其分为5类：东移型、东北移型、东南移型、西移型和少动型;东移型、东南移型、少动型低涡生成个数的峰值在6月,东北移型和西移型低涡生成个数的峰值在7月。夏季5类长生命史四川盆地低涡的结构和降水合成场表明：从发展强度看,东北移型最强,少动型最弱。从成熟期垂直结构看,除西移型外,低涡均随高度向西北或向西倾斜,在对流层低层为冷性结构,中层为暖性结构;东移型、东北移型、西移型低涡的正涡度区在垂直方向伸展更高;除东南移型、西移型低涡的强上升区与其中心重合外,其余类型位于其中心东侧。从降水特征看,除西移型外,其余类型低涡的降水中心均位于其移动路径东侧或东北侧,其中东北移型低涡成熟期6 h累计降水量最大。四川盆地低涡的强上升区、相对湿度大值区、位于对流层低层和中层的辐合辐散中心与降水所在位置有很好的对应关系,各物理量场相互作用共同促进低涡发展。     

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.     

“12.7.21”西南涡极端强降雨的成因分析

利用常规观测资料、ECMWF分析场、区域自动站、多普勒雷达及SWAN系统产品等资料对2012年7月21日西南涡暴雨过程及盘龙极端强降雨进行分析。分析发现：此次过程是“北槽南涡”形势下,地面冷空气触发西南涡其东侧辐合上升运动强烈发展,高层强辐散,因而产生了对流性暴雨天气过程;冷空气从西侧侵入西南涡是925 hPa “S”形冷锋形成的直接原因,也是地面辐合线形成的重要因素;极端短时强降雨就发生在西南涡东侧中尺度雨带的中部偏北区域,有地面辐合线相配合,降雨最强时MCC冷云中心TBB达最低值。雷达回波表明：西南涡两侧冷暖空气的交绥促进了β中尺度气旋式环流的形成;偏南风低空急流为强降雨提供了充足的水汽,增强了中低层的垂直风切变,有利于强降水超级单体风暴的发展和维持;盘龙的极端短时强降雨是β中尺度气旋式环流中,伴随有深厚中气旋的强降水超级单体风暴在环流中心附近持续发展的结果。     

应用MJO制作长江流域月降水预测的试验研究

用MJO指数RMM1、RMM2、振幅 1—25日平均代替月平均,用上月月平均RMM1和RMM2、振幅构造为右场,下月长江流域降水场为左场,SVD分析两场的关联,借助最优化技术,在降水场预测距平与实况距平同号总站数最大意义下确定系数,建立估计公式,由右场时间系数估计左场时间系数,最后反演降水场。尽管多数的月第一模态相关并不显著,但实际预测效果较好。     

近40年来塔什干低涡活动特征的统计分析

利用1971-2010年NCEP/NCAR逐日再分析资料,根据塔什干低涡定义,分析了塔什干低涡的时空分布特征、移动路径及其对南疆天气的影响.结果表明:(1)1971-2010年,塔什干低涡过程平均每年出现7.95次,成熟期生命史平均为3.1天,4天以上的仅有13.5％; (2)4-6月和9-10月是塔什干低涡活动的两个高峰期,其中5月出现次数最多,其次是10月和6月;(3)塔什干低涡频次的年代际变化呈抛物线型,1970-1980年代由78次增加到83次,之后逐渐减少,年低涡频次存在7年左右的显著振荡周期,同时具有1 3年的次振荡周期;(4)塔什干低涡活动有两个高频中心,分别位于67.5°E,40.0°N和72.5°E,35.0°N,移动路径以偏东方向为主,占84％,西退塔什干低涡仅有5.7％;造成南疆显著降水天气的塔什干低涡占其总数的23.3％,夏季此类低涡所占比例最高,达41.2％.     

Intraseasonal Oscillation in Global Ocean Temperature Inferred from Argo

The intraseasonal oscillation(ISO;14-97-day periods) of temperature in the upper 2000 m of the global ocean was studied based on Argo observations from 2003-2008.It is shown that near the surface the ISO existed mainly in a band east of 60 E,between 10 S and 10 N,and the region around the Antarctic Circumpolar Current(ACC).At other levels analyzed,the ISOs also existed in the regions of the Kuroshio,the Gulf Stream,the Indonesian throughflow,the Somalia current,and the subtropical countercurrent(STCC) of the North Pacific.The intraseasonal signals can be seen even at depths of about 2000 m in some regions of the global ocean.The largest amplitude of ISO appeared at the thermocline of the equatorial Pacific,Atlantic and Indian Ocean,with maximum standard deviation(STD) exceeding 1.2 C.The ACC,the Kuroshio,and the Gulf Stream regions all exhibited large STD for all levels analyzed.Especially at 1000 m,the largest STD appeared in the south and southeast of South Africa-a part of the ACC,with a maximum value that reached 0.5 C.The ratios of the intraseasonal temperature variance to the total variance at 1000 m and at the equator indicated that,in a considerable part of the global deep ocean,the ISO was dominant in the variations of temperature,since such a ratio exceeded even 50% there.A case study also confirmed the existence of the ISO in the deep ocean.These results provide useful information for the design of field observations in the global ocean.Analysis and discussion are also given for the mechanism of the ISO.