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1.
通过对热带太平洋上层XBT温度资料分析,探讨了对厄尔尼诺(El Nino)事件发生起重要作用的西太平洋暖池区次表层海温变暖异常的变化规律,揭示了影响西太平洋暖池区次表层海温变暖异常的形成机制.分析表明:西太平洋暖池区的次表层海温异常变暖与赤道太平洋的北赤道流(10°N)的海温异常存在密切关系.在El Nino事件发生的前期,位于赤道中东太平洋的异常暖水沿北赤道流温跃层潜沉向西太平洋暖池区输送,在西太平洋暖池堆积并向赤道西太平洋扩展,当异常暖水达到一定强度,并在大气的强迫下,异常暖水沿温跃层东传至赤道中东太平洋并上浮于海面,最终导致El Nino事件的爆发.北赤道流的异常海温西传是导致西太平洋暖池区次表层海温异常的重要机制,是导致El Nino事件发生的关键. 相似文献
2.
ENSO-7赤道西太平洋异常纬向风所驱动的热带太平洋次表层海温距平的循环 总被引：13，自引：0，他引：13
近几年的一系列分析研究表明，ENSO与异常东亚冬季风之间有相互影响，持续的强（弱）东亚冬季风通过引起赤道西太平洋地区的西（东）风异常对El Niño/La Niña的发生起着重要作用；赤道太平洋次表层海温异常（SOTA）的年际变化（循环）与ENSO发生有密切关系；ENSO的真正源在西太平洋暖池，暖池正（负）SOTA沿赤道温跃层东传到东太平洋，便导致El Niño/La Niña的爆发；在暖池正（负）SOTA沿赤道东传的同时，有负（正）SOTA沿10°N和10°S纬度带向西传播，从而构成SOTA的循环；热带太平洋SOTA循环的驱动者是赤道西太平洋的异常纬向风。进而可以认为：ENSO实质上是主要由异常东亚季风引起的赤道西太平洋异常纬向风所驱动的热带太平洋次表层海温距平的年际循环。 相似文献
3.
应用热带太平洋上层XBT温度资料,分析探讨了西太平洋暖池区次表层海温冷暖异常信号的变化规律,揭示了影响西太平洋暖池区次表层海温冷变异常的信号通道。分析表明,西太平洋暖池区的次表层海温异常变冷与太平洋北赤道流的海温冷异常信号西传有重要关系。北赤道流的海温异常冷(暖)信号是沿温跃层由赤道中东太平洋潜沉向西太平洋暖池区传播,与西太平洋次表层海温异常(冷)暖信号向赤道中东太平洋传播构成了热带海洋信号的气旋式"环流通道"。在这一"环流通道"中,北赤道流的海温异常信号西传是导致西太平洋暖池区及西太平洋次表层海温异常的重要机制,是影响厄尔尼诺(ElNino)和拉尼娜(LaNina)事件发生的关键。 相似文献
4.
应用TOGA-TAO实测海流资料(ADCP)和SODA同化海流和海温资料,分析探讨了赤道太平洋潜流的季节和年际变化特征,以及与赤道异常暖水东传的内在联系.揭示了El Nino事件中异常暖水东传的物理机制.结果表明,赤道太平洋潜流具有明显的季节变化和年际变化特征.潜流的垂直最大深度可由海表层至300~400 m,其多年平均最大流速可达100 cm/s.潜流最大中心的纬向变化位置基本维持在160°W-130°W之间.在年际变化中,赤道潜流变化特征非常明显,尤其是在El Nino事件发生过程中,赤道潜流出现明显的加强现象.其最大流速可达140 cm/s以上.在西太平洋暖池区域次表层暖水东传之前,位于中东太平洋次表层的赤道潜流就已出现加强,其最大流速中心沿温跃层不断加强和东移,“引导”来自西太平洋暖池区域次表层的异常暖水向东传播.因此,可以认为西太平洋暖池区域异常暖水的东传与赤道潜流的强度和东传存在密切关系,也就是说在El Nino事件中,赤道潜流的变化是导致西太平洋暖池区域次表层异常暖水东传的重要机制. 相似文献
5.
利用Scripps海温再分析资料,对赤道印度洋0～400m深度范围内海温变化和偶极子异常变化特征进行了初步分析。结果显示,赤道印度洋上层海温呈现西低东高,而次表层以下海温则为西高东低。同时发现,温跃层是赤道印度洋上、下层很好的分界面。温跃层之上海温变化受海气相互作用明显,之下海温变化主要受海洋自身的运动影响。赤道印度洋偶极子现象存在于各个深度,其偶极子指数变化存在半年周期,季节变化表现为双峰双谷型,并从深层（400m）向表层传递。分析发现,海气相互作用不是表层赤道印度洋偶极子变化的决定因素。较深层偶极子变化决定于海洋自身的运动变化特征（如洋流）,并向上层传输,进而影响上层偶极子的异常变化。赤道印度洋偶极子指数由西印度洋和东印度洋海温变化共同制约,但西印度洋海温变化起主导作用,东印度洋仅起到加强或减弱偶极子强度变化的作用。 相似文献
6.
《地球科学进展》2017,(4)
火山活动是影响全球气候变化的重要自然因子。在年代际预测试验中加入火山气溶胶强迫会带来火山爆发后短期内气候响应回报技巧的改变。基于耦合气候系统模式FGOALS-s2的中国科学院大气物理研究所年代际气候预测试验(DP-EnOI-IAU试验)结果,分析了火山活动对太平洋海温年代际预测技巧的影响。DP-EnOI-IAU试验引入了平流层火山气溶胶的辐射外强迫变化,在模拟的1960—2005年共发生4次强的热带火山爆发事件。结果表明,DP-EnOI-IAU试验在多数年份对太平洋海温具有显著的预测技巧,但预测技巧在1982年El Chichon火山爆发和1991年Pinatubo火山爆发后显著下降。模式对火山爆发后ENSO位相的模拟偏差导致了其对太平洋海温年代际预测技巧的下降。对于1982年El Chichon火山爆发,在火山爆发峰值时期和第3年冬季,赤道中东太平洋均表现出与观测相反的海温型响应,使得DP-EnOI-IAU试验对太平洋海温的年代际预测技巧显著下降。在1991年Pinatubo火山爆发后的秋冬季和第3年冬季,观测和模拟的热带海温型亦相反,模式对1991年火山爆发后太平洋海温的预测技巧降低。相对于1982年El Chichon和1991年Pinatubo火山爆发,模式对1963年Agung火山爆发后热带海温型响应的模拟与观测较为一致,此次火山爆发没有带来太平洋海温预测技巧的显著下降。 相似文献
7.
《地球科学进展》2017,(4)
海洋同化系统为年代际预测试验提供初值,其性能可能会影响年代际预测技巧,因此评估其对重要年代际变化现象的模拟能力非常必要。观测发现,东亚夏季风(EASM)和前冬厄尔尼诺—南方涛动(ENSO)的关系在1970s末加强,随后在1990s中期后减弱。基于FGOALS-s2耦合气候模式的海洋同化系统评估了其对这2次年代际变化的模拟能力。结果表明,决定模式能否再现EASM和前冬ENSO关系的年代际变化有2个重要因素:(1)与前冬ENSO有关的夏季印度洋—太平洋海温型的年代际变化;(2)模式西北太平洋反气旋对热带海温的响应偏差。模式中西北太平洋反气旋与东北印度洋的暖海温关系稳定,当1970s末前冬ENSO对夏季印度洋海温影响显著增强时,模式能够模拟出北印度洋降水以及赤道东印度洋至海洋大陆上空Kelvin波的增强,从而可再现EASM与前冬ENSO关系的增强;而1990s中期后模式中与前冬ENSO有关的东北印度洋海温异常进一步增强,与观测相反,使得模式未能再现观测中EASM与前冬ENSO关系的减弱。此外,1990s中期后模式对夏季中太平洋冷海温异常的Rossby波响应存在较大偏差,是其未能再现此次年代际变化的另一个原因。研究表明,与ENSO有关的热带印太海温的年代际变化预测水平和模式对海温的响应偏差将在一定程度上制约模式对EASM与ENSO关系的年代际预测能力。 相似文献
8.
用因子分析及方差最大原则下的正交旋转技术,计算并识别长江中下游汛期(5～9月)降水场的四个空间高载荷区及相对应的因子得分系数.它们的空间、时间变化,反映了长江中下游区域的实际降水特点.赤道东太平洋海温、区域平均海温及ENSO事件都与高载荷区的汛期降水有一定的联系,所得结果可作为汛期降水短期气候预报的参考因子. 相似文献
9.
作为全球接受太阳辐射最多、表层海水温度最高的区域,西太平洋暖池区通过厄尔尼诺-南方涛动(El Niño-Southern Oscillation,ENSO)和季风等过程影响着全球气候的变化。越来越多的沉积记录证明,在地质历史时期西太平洋暖池也存在类似于现代ENSO过程的“类ENSO式”变化。而目前类ENSO式变化与冰期—间冰期旋回之间的响应关系和驱动机制及其与东亚季风的关联仍存在争议。本文利用位于暖池核心区的B10岩心浮游有孔虫氧同位素、Mg/Ca(质量分数比)和黏土矿物参数重建了暖池区氧同位素8期以来的古气候记录,并结合已有的热带海表温度记录、中国石笋氧同位素和南大洋地区海表温度记录,研究了西太平洋暖池冰期旋回中类ENSO状态的演化规律及其与东亚季风的关系,并探讨了暖池区类ENSO演化的驱动机制。结果发现:冰期时,西太平洋暖池区温跃层变浅,赤道东、西太平洋温差减小,同时,东亚夏季风减弱,暖池区降水量相对减少,与现代El Niño时期气候态类似;间冰期时,西太平洋暖池区温跃层加深,赤道东、西太平洋温差增大,东亚冬夏季风增强,暖池区降水量相对增加,与现代La Niña时期气候态类似。频谱分析结果表明,西太平洋暖池区海表温度的变化具有偏心率周期(96 ka)。冰消期时,低纬度太阳辐射量的增加,增大了纬向上的SST梯度,并使得次表层海水储存了更多的热量,积累的热量会通过调节次表层环流向暖池区的热传输,最终调控赤道太平洋地区Walker环流强度和ENSO活动的长期变化。而冰期时,南大洋地区降温所引起的东南信风和大洋环流异常可能对类ENSO式起到调控的作用。 相似文献
10.
文章利用美国NASA的GISS海气耦合模式,研究了14MaB.P.时期与现代情景下的澳大利亚板块不同位置对赤道太平洋的影响。结果表明:14MaB.P.澳大利亚板块位置较现代偏南时,海洋次表层南赤道海水穿过印度尼西亚通道直接进入印度洋,注入赤道潜流的南赤道海水减少,使得赤道潜流主要来源于北赤道海水,造成赤道太平洋海温比现在冷,其中以赤道西太平洋海温降低幅度最大。而在海洋近表层赤道中东太平洋地区,由于进入海洋的净能量增加和西向风应力加强的共同作用,使得14MaB.P.时海温较之现代情景下要低0.2℃左右。此外,14MaB.P.澳大利亚板块较现代偏南时,赤道太平洋地区的降水量少于现代。 相似文献
11.
中国气温变化的两个基本模态的诊断和模拟研究 总被引：11，自引：0，他引：11
我国地域辽阔，气候复杂多变，在全球变暖的背景下研究中国近百年来的气温变化具有重要的意义。为此我们重建了中国东部71个站1880—2004年四季气温距平序列。通过EOF分析发现了中国气温变化的2种最基本的模态：东部一致变化和关内关外相反变化。这2种模态不随季节变化，而且在不同时期也是稳定的。通过研究这2种模态与变暖趋势的关系发现，20世纪80年代以来的变暖主要是由于第一模态在该时期持续的正位相增强造成的；而20世纪20~40年代的变暖主要是由于第二模态所呈现的正位相所造成的。此外，我们检验了这2种模态在大气环流模式（CAM）中的表现。结果表明：121年（模式中1880—2000年）的集合模拟在一定程度上可以重现第一模态的变化，而第二模态则仅在冬季表现明显。最后，以冬季为例，利用1880—2004年重建及观测的500 hPa高度场资料，通过合成分析进一步研究了这2种模态的环流机制：第一模态正位相对应纬向环流增强，表现在地面气温分布上为东部一致变暖。而负位相则对应东亚大槽加深，东部地区一致变冷。第二模态正位相对应的环流分布则为从东亚北部到阿留申为负距平，东亚到北太平洋中纬度为正距平；对应地面气温分布为关内变暖关外变冷。负位相时环流分布基本相反。这样的环流机制得到了模式研究的支持。 相似文献
12.
ENSO事件对长江上游1470-2003年旱涝灾害影响分析 总被引：10，自引：1，他引：9
对长江上游旱涝灾害时间序列(1470-2003年)及SST指数序列(1868-2003年)作统计相关与谱分析,探讨了长江上游旱涝灾害与ENSO事件的遥相关关系.结果表明:长江上游旱涝灾害主周期要大于ENSO事件的主周期,前者主周期主要为16.69a,5.09a以及10.47a,而后者主周期主要为5a,～10～12年以及～10a.交叉谱分析结果表明,长江上游旱涝灾害与SST在约5a以及约10～12a周期上呈现出显著的相关性.可以认为ENSO事件发生周期与生存周期的长短直接影响着长江上游旱涝灾害发生的周期与频率,并在5a以及10～12a的周期上表现出高的统计相关性.SST指数与长江上游旱涝灾害相关分析表明,ElNiño事件的发生使长江上游发生旱灾机率增大,而LaNiña事件的发生则使长江上游发生涝灾的机率增大. 相似文献
13.
Anomalous sea level, anomalous observed dynamic height (0/400 db) and anomalous model dynamic height are examined at the locations
of 13 island sea level stations in the tropical Pacific for each bimonth of the four year period 1979 to 1982. Starting in
1981, the anomalous dynamic height data show off-equatorial Rossby waves propagated toward the W boundary of the Pacific basin.
At the W boundary, the model Rossby wave activity was found to have excited coastally trapped Kelvin-Munk waves which transmitted
the anomalous dynamic height equatorward. At the equator, coastally trapped wave activity excited eastward propagating equatorial
Kelvin waves, yielding a pair of anomalous peaks in dynamic height variability in the E equatorial Pacific associated with
the 1982–1983 ENSO event. The evolution of the peaks in dynamic height associated with the Rossby and Kelvin wave activity
reflects the redistribution of observed upper-ocean heat content in the W tropical Pacific, providing a qualitative hindcast
for the 1982–1983 ENSO event.
In consequence of these results, and the results of a related study (Inoue et al. 1985), the redistribution of both observed
and model heat content, as evidenced in dynamic height in the W Pacific during the 23-year period 1964–1985, is examined for
its ability to hindcast and forecast ENSO events in this period. Complex EOF analysis is applied to the Onset Phase of ENSO
events occurring in 1968–69, 1972–73, 1976–77, and 1982–83; it is used to determine the characteristic redistribution of heat
content (dynamic height) prior to the Mature Phase of ENSO events. This analysis found both model and observed dynamic height
in the N hemisphere to be characterized by wind-driven, westward propagating, baroclinic Rossby wave activity, having a remarkably
stable period of 3 years over the 23-year period. The complex time series associated with these first spatial eigen-functions
are used to construct observed and model hindcast indices that yield high values one year prior to the Mature Phase of ENSO
events of the period. These indices achieve these values due to the incidence upon the Philippine coast in fall/winter of
a positive anomaly in dynamic height propagating from the east at nondispersive Rossby long wave speeds. 相似文献
14.
Records from South America show that modern ENSO (El Nino-Southern Oscillation) did not exist 7000 cal yr B.P. and has developed progressively since then. There has been little information available on oceanic conditions in the eastern equatorial Pacific (EEP) to constrain explanations for ENSO onset. We report quantitative observations on thermocline and mixed-layer conditions in the EEP during ENSO start up. We found important changes in both the thermocline and the mixed layer, indicating increased upwelling of cooler waters since 7000 cal yr B.P. This resulted from change in the source and/or properties of waters supplying the Equatorial Undercurrent, which feeds upwelling along the equator and the Peru margin. Modeling shows that ENSO is sensitive to subsurface conditions in the eastern equatorial Pacific and that the changes in the thermocline we observed were driven by extratropical processes, giving these a role in conditioning the development of ENSO. This is in contrast to models that call for control of equatorial Pacific oceanography by tropical processes only. These infer stronger upwelling and cooler surface waters for the EEP during the mid-Holocene, which is not supported by our results. 相似文献
15.
ENSO(厄尔尼诺-南方涛动)事件的发生会影响区域气候变化。通过对青海东部地区5个站点1959~2005年的降水、气温资料、干燥度和海表温度距平(SSTA)与南方涛动指数(SOI)的月序列进行相关性分析和周期性谱分析,探讨了区域气候变化与ENSO事件的关系。结果表明,1959~2005年青海省东部地区气候趋于暖干,并且冬春季变化趋势显著;暖事件的发生对该区域降水、气温及干燥度的变化影响较大,且气温对ENSO事件的响应要大于降水;ENSO事件对该区域的气候变化有两到三个月的影响期,EI Nino事件的发生对当月的影响较大,而La Nina事件的发生对该区域有两到三个月的持续影响期;降水距平及气温距平与ENSO事件存在短期相同的变化趋势,且该地区气候变化受南方涛动影响明显。 相似文献
16.
Muhammad Mubashar Dogar Fred Kucharski Syed Azharuddin 《Journal of Earth System Science》2017,126(2):30
ENSO is considered as a strong atmospheric teleconnection that has pronounced global and regional circulation effects. It modifies global monsoon system, especially, Asian and African monsoons. Previous studies suggest that both the frequency and magnitude of ENSO events have increased over the last few decades resulting in a need to study climatic impacts of ENSO magnitude both at global and regional scales. Hence, to better understand the impact of ENSO amplitude over the tropical and extratropical regions focussing on the Asian and African domains, ENSO sensitivity experiments are conducted using ICTPAGCM (‘SPEEDY’). It is anticipated that the tropical Pacific SST forcing will be enough to produce ENSO-induced teleconnection patterns; therefore, the model is forced using NINO3.4 regressed SST anomalies over the tropical Pacific only. SPEEDY reproduces the impact of ENSO over the Pacific, North and South America and African regions very well. However, it underestimates ENSO teleconnection patterns and associated changes over South Asia, particularly in the Indian region, which suggests that the tropical Pacific SST forcing is not sufficient to represent ENSO-induced teleconnection patterns over South Asia. Therefore, SST forcing over the tropical Indian Ocean together with air–sea coupling is also required for better representation of ENSO-induced changes in these regions. Moreover, results obtained by this pacemaker experiment show that ENSO impacts are relatively stronger over the Inter-Tropical Convergence Zone (ITCZ) compared to extratropics and high latitude regions. The positive phase of ENSO causes weakening in rainfall activity over African tropical rain belt, parts of South and Southeast Asia, whereas, the La Niña phase produces more rain over these regions during the summer season. Model results further reveal that ENSO magnitude has a stronger impact over African Sahel and South Asia, especially over the Indian region because of its significant impact over the tropical Atlantic and the Indian Ocean through Walker circulation. ENSO-induced negative (positive) NAO-like response and associated changes over Southern Europe and North Africa get significantly strong following increased intensity of El Niño (La Niña) in the northern (southern) hemisphere in the boreal winter (summer) season. We further find that ENSO magnitude significantly impacts Hadley and Walker circulations. The positive phase of ENSO (El Niño) overall strengthens Hadley cell and a reverse is true for the La Niña phase. ENSO-induced strengthening and weakening of Hadley cell induces significant impact over South Asian and African ITCZ convective regions through modification of ITCZ/monsoon circulation system. 相似文献
17.
It has been shown that large-scale weather patterns in both the tropical South Pacific (El Niño-Southern Oscillation, or ENSO, events) and the North Pacific (Pacific-North American, or PNA, patterns) have strong teleconnection effects on the air, ice, and ocean environments of the Bering Sea. This signal apparently comes via the atmosphere and not the ocean. The connection between variability of the Bering Sea and the ENSO and PNA appears to be the winter position of the Aleutian Low. Interannual variability in air temperatures, ice cover, and surface winds in the Bering Sea generally are in phase with each other, whereas sea-surface temperatures (SST) tend to lag these variables by 1–3 months. These Bering Sea time-series are significantly correlated with the Southern Oscillation Index (SOI) time-series (an indicator of ENSO events) when the Bering sea data are lagged behind the SOI for up to 18 months. The correlations suggest that warming in the Bering Sea follows negative anomalies in the SOI (i.e., El Niño events). Cooling in the Bering Sea tends to follow positive anomalies (i.e., precursors of El Niños) in the SOI. Maximal correlations for the PNA also lag the SOI by a mouth or two.Analyses of variance indicate that the SOI can explain 30–40% of the variability in the Bering Sea. Stepwise multiple regressions can explain up to 54% of the variation in air temperatures, up to 39% of the variation in sea ice cover, and up to 46% of the variation in SST in the Bering Sea. PNA and SOI were significant variables only in the equation for air temperatures, indicating a close relationship between them and the atmosphere in the Bering Sea and suggesting that energy is transmitted to the water and ice via the atmosphere. The three variables airtemps, ice, and SST were significant each time they were used as independent variables, indicating a rapid and strong feedback relationship among them.Three ENSO events have occurred since the mid-1970s, but none have been typical. There have been either two positive SOI anomalies preceding an El Niño or there have been none preceding an El Niño. When there has been a positive anomaly, ice cover has been above normal, but neither a positive anomaly nor above-normal ice has occurred in the past two ENSO events. An ice retreat has occurred any time there has been an ENSO event, except in the case of the great El Niño of 1982–1983; the anomalous position of the Aleutian Low at that time explains the lack of response of the ice. Finally, one ice retreat occurred that was unrelated to an ENSO event, but was related to a PNA event. 相似文献
18.
The stability of a simple coupled ocean-atmosphere system similar to the one studied by Hirst with general ocean thermodynamics
is investigated in which the atmospheric heating is determined by sea surface temperature anomalies as well as the convergence
feedback (low level moisture convergence by the waves themselves). It is shown that the unstable coupled mode found by Hirst
(UH mode) is profoundly modified by the convergence feedback. The feedback increases the unstable range of the UH mode and
can increase its growth rate several folds. The maximally growing UH mode can become westward propagating for certain strength
of convergence feedback. If the convergence feedback strength exceeds a critical value, several new unstable intraseasonal
modes are also introduced. These modes are basically ‘advective’ modes. For relatively weak strengths of the convergence feedback
the growth rates of these modes are smaller than that of the UH mode. As the atmosphere approaches ‘moist neutral’ state,
the growth rates of these modes could become comparable or even larger than that of the UH mode. It is argued that these results
explain why the El Nino and Southern Oscillation (ENSO) signal is clear in the eastern Pacific but not so in the western Pacific
and they may also explain some of the differences between individual ENSO events. Our results also explain the aperiodic behaviour
of some coupled numerical models. Importance of this process in explaining the observed aperiodicity of the ENSO phenomenon
is indicated. 相似文献