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| 1 | Strengthening of the boreal winter Hadley circulation and its connection with ENSO显示文摘Empirical orthogonal function (EOF) analysis is carried out for the year-to-year variability of the boreal winter (DJF) mass stream function of the mean meridional circulation (MMC) during the period 1948—2005. The results demonstrate that it is dominated by the equatorially asymmetric and symmetric modes. Further analysis shows that the former mode is linked with the boreal winter Hadley cell mainly on the decadal time-scale, and the latter on the interannual time-scale. The asymmetric mode index (AMI) with a clear upward trend contributes to the decadal strengthening of the boreal Hadley circulation, and is closely correlated with the tropical SST warming, especially in the region of Indo-west Pacific warm pool (INWP). Furthermore, the AMI also contributes to the abrupt change of the correlation coefficient between the boreal Hadley circulation and ENSO after 1976. The symmetric mode index (SMI) with robust and stable linkage with ENSO shows a significant interannual variability, suggesting that the variability of the Hadley circulation is mainly associated with ENSO on the interannual time-scale. | Ma Jie Li Jianping | 2007 | Progress in Natural Science:Materials International2007，17，11： | 10 |
| 2 | LOCALIZED HADLEY CIRCULATION AND ITS LINKAGE TO PACIFIC SSTA显示文摘The 1979-2001 ERA-40 monthly mean meridional winds are used to calculate the mass streamfunctions in the monsoon region (60-140° E) and Nio zone (160° E-120° W),with which the climate characteristics and intensity variation of the localized Hadley circulation (LHC) are analyzed over the two regions and the linkage of this LHC to Pacific SST is explored.Evidence suggests as follows.1) The climatological LHC is stronger in the monsoon than in the Nio zone,with its position in the former northward of the latter,especially in the summer half-year.The resulting difference is due mainly to the land-sea heterogeneous distribution and the existence of a cold pool in the equatorial eastern Pacific.2) The LHC experiences a distinct interannual variability in intensity and during 1979-2001 the LHC strength of the two regions changes broadly in an anti-phase manner.3) The LHC has its intensity associated closely with Pacific SST in such a way that its strength anomaly in the monsoon (Nio) band in January is correlated negatively (positively) with the SSTA over the all-Nio (1-4) zone (ANZ) in the equatorial middle and eastern Pacific but positively (negatively) correlated to SSTA in the C-shaped area that surrounds the ANZ.The pattern of July is in rough agreement with that of January,except for more feeble correlativity in July,especially over the monsoon region;4) The ENSO episode has different impacts on the LHC vigor in the two regions.With the occurrence of an El Nio,the LHC is weakened (strengthened) in the monsoon (Nio) region,and the reversal takes place during the La Nia year,with greater anomaly in the Nio area. | 秦育婧 王盘兴 | 2011 | Journal of Tropical Meteorology2011，17，4： | 2 |
| 3 | THE DOUBLE-LAYER STRUCTURE OF THE HADLEY CIRCULATION AND ITS INTERDECADAL EVOLUTION CHARACTERISTICS显示文摘Based on the three-pattern decomposition of global atmospheric circulation(TPDGAC), this study investigates the double-layer structure of the Hadley circulation(HC) and its interdecadal evolution characteristics by using monthly horizontal wind field from NCEP/NCAR reanalysis data from 1948—2011. The following major conclusions are drawn: First, the double-layer structure of the HC is an objective fact, and it constantly exists in April,May, June, October and November in the Southern Hemisphere. Second, the double-layer structure is more obvious in the Southern than in the Northern Hemisphere. Since the double-layer structure is sloped in the vertical direction, it should be taken into consideration when analyzing the variations of the strength and location of the center of the HC.Third, the strength of the double-layer structure of the HC in the Southern Hemisphere consistently exhibits decadal variations with a strong, weak and strong pattern in all five months(April, May, June, October, and November), with cycles of 20-30 a and 40-60 a. Fourth, the center of the HC(mean position of the double-layer structure) in the Southern Hemisphere consistently and remarkably shifts southward in all the five months. The net poleward shifts over the 64 years are 5.18°, 2.11°, 2.50°, 1.79° and 5.76° for the five respective months, with a mean shift of 3.47°. | 成剑波 胡淑娟 丑纪范 | 2018 | Journal of Tropical Meteorology2018，24，2： | 1 |
| 4 | Interannual Variability of the Hadley Circulation Associated with Tropical Pacific SST Anomaly显示文摘The seasonal and interannual variability of zonal mean Hadley circulation are analyzed, and the important effects of sea surface temperature(SST), especially the tropical Pacific SST, on the meridional circulation are discussed. Following results are obtained: 1) the Hadley circulation presents a single clockwise(anticlockwise) cross-equator circulation in the Northern(Southern) Hemisphere winter,while it is a double-ring-shaped circulation quasi-symmetric about the equator in spring and autumn. The annual mean state just indicates the residual of the Hadley cell in winter and summer. 2) The first mode of interannual anomalies shows a single cell crossing the equator like the climatology in winter and summer but with narrower width. The second mode shows a double ring-shaped cell quasi-symmetric about the equator which is similar to the Hadley cell in spring or autumn. 3) Vertical motion of the Hadley circulation is driven by sea surface temperature(SST) through latent and sensible heat in the tropics, and the interannual anomalies are mainly driven by the SST anomaly(SSTa) in the tropical Pacific. 4) The meridional gradient of SSTa is well consistent with the lower meridional wind of Hadley circulation in the interannual part. For the spatial distribution, the meridional gradient of SSTa in the Pacific plays a major role for the first two modes while the effects of the Indian Ocean and the Atlantic Ocean can be ignored. | GONG Xiaoqing WANG Qi LIU Yulong | 2015 | Journal of Ocean University of China2015，14，4： | 1 |
| 5 | 热带月平均风场谱结构的傅立叶分析Ⅰ——气候风场分析显示文摘用风场傅立叶分析方案,分析了NCEP/NCAR再分析资料的热带(30°S^30°N)850、200 hPa气候风场V8 50、V2 00的谱结构,讨论热带风场定常波的成因,以弥补热带气候风场此类分析工作的空白。研究结果表明,(1)有低维、低阶特征,|m|=0,4-、0,3-波对月8 50、2 00的累积模方拟合率年均达90%、98%。(2)纬向平均分量0最重要,它对8 50、2 00的单波拟合率ρ0年均达52%、85%。850 hPa0主要由北、南半球的两支信风带构成,冬半球强、夏半球弱,轴线位置与所在半球Hadley环流中心对应;200 hPa0由强的外热带西风带和弱的内热带东风带构成。0的季节变化850 hPa层明显强于200 hPa,北半球明显强于南半球。(3)风场定常波的最大波分量全年两层均为|1|*,它对850*、200*的拟合率ρ|*1|年均达39%、55%;ρ|1|*作年双周振荡,北半球夏、冬季达极大,秋、春季达极小。次大波分量在北半球冬、夏季时同为3、2波,过渡季节也以3、2波为主(10—12月850*4波是例外)。(4)1、7月射出长波辐射定常波OLR*最大、次大波与同期V*相同,1月为1、3波,7月为1、2波;OLR*重要波分量上的极值区与*相应波分量散度场的垂直配置符合动力学原理。(5)7月青藏高原及以东以南的广阔区域,*的主要分量|1|*、|2|*同为下层辐合、上层辐散,1OLR*、2OLR*同为负值,是同纬度上最有利于降水和潜热释放的气候区。 | 吴幸毓 王盘兴 周国华 华文漪 李丽平 | 2012 | 热带气象学报2012，28，1： | 0 |
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