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1.
基于CMIP5多模式中的历史情景与全球变暖情景资料以及观测海温数据,利用EOF分析,回归分析、功率谱分析等方法对北太平洋区域冬季海—气耦合系统进行了研究,进而分析了全球变暖背景下太平洋年代际振荡（PDO）时空特征的变化。通过对比观测资料中1934年前后的PDO时空特征,发现在全球变暖的背景下,PDO强度得到加强,PDO模态的频率向高频移动（周期变短）;再用泰勒图分析方法和功率谱分析方法评估13个CMIP5模式对20世纪太平洋年代际振荡（PDO）的模拟能力;在此基础上,选取评估良好以上的9种模式对比分析不同增暖情景下的PDO时空特征变化,发现模式中PDO对全球变暖的响应与观测结果基本一致。 相似文献
2.
本文利用1958～2018年期间海表面温度（SST）异常和湍流热通量异常变化的关系,探讨了其与北太平洋年代际振荡（PDO）相关的年际和年代际时间尺度上在不同海域的海气相互作用特征。结果表明:在年际尺度上,黑潮—亲潮延伸区（KOE）表现为显著大气强迫海洋,赤道中东太平洋表现为显著海洋强迫大气;在年代际尺度上,PDO北中心表现为大气强迫海洋,加利福尼亚附近则表现为显著海洋强迫大气。进一步分析表明:加利福尼亚附近区域是北太平洋准12年振荡的关键区域之一,与PDO准十年的周期类似,加利福尼亚附近的冷（暖）海温对应其上有反气旋（气旋）型环流,赤道中太平洋海水上翻和北太平洋东部副热带区域经向风应力的变化是北太平洋准12年振荡的另外两个重要环节。 相似文献
3.
对1955—1998年的夏季次表层(0~400 m)海温进行了EOF分解,对比分析了中低纬太平洋夏季次表层海温的年代际变化特征。结果表明:中纬太平洋夏季次表层海温有2种年代际分布模态:0~160 m表现为PDO型,200~400 m表现为全区一致型;低纬太平洋夏季次表层海温有3种年代际分布模态:0~60 m和300~400 m为全区一致型,80~240 m为东西反向型。太平洋夏季次表层海温异常的年代际变化在中低纬都存在从上而下的时间滞后;而同一层中低纬太平洋夏季次表层海温年代际突变的时间也不一致。 相似文献
4.
利用第五次耦合模式比较计划（CMIP5）40个模式的模拟资料和分类集合的方法,评估了耦合模式对20世纪太平洋年代际振荡（PDO）特征的模拟能力。结果表明,CMIP5多数模式对PDO周期有着较好的刻画能力,能模拟出PDO的年代际变化周期。模式对PDO模态空间特征的模拟能力存在较大差异,小部分模式模拟效果较差。进一步的分析表明,对PDO模态模拟较好的第1类模式,能较好地再现热带太平洋与北太平洋海表温度异常（SSTA）年代际变化间的关系,而且热带太平洋SSTA通过大气遥相关影响北太平样海表温度的过程也模拟的较成功。对PDO模态模拟差的模式,不能合理模拟出热带太平洋SSTA对北太平洋海表温度影响的遥相关过程。以上研究也证实了热带太平洋地区海表温度的年代际变率对北太平洋海表温度年代际变率的重要影响,热带太平洋SSTA对北太平洋SSTA的影响是通过大气遥相关实现的。利用CMIP5中等排放情景模拟结果,分析了第1类模式预估的北太平洋年代际变率的特征,发现21世纪北太平洋年代际变率的主要模态为一致的正异常分布且呈现明显的上升趋势,第二模态则表现为类似于20世纪典型PDO的马蹄型SSTA分布。 相似文献
5.
利用小波变换和小波互相关分析法对1901—2000年的北极涛动（Arctic Oscillation,AO）、北大西洋多年代际振荡（Atlantic Multidecadal Oscillation,AMO）和北太平洋年代际振荡（Pacific Decadal Oscillation,PDO）的年代际振荡关系进行研究,并利用1 000 hPa高度场合成分析进行验证。结果表明,三个气候模态均有明显的多年代际尺度的振荡特征,且它们在各特征时间尺度上的振荡相关性存在显著区别,主要表现为:在60 a尺度上,AO超前PDO约4 a正相关,AO滞后AMO约12 a负相关;在20～30 a尺度上,AO超前PDO约12 a正相关;在30 a尺度上,AO超前AMO约8 a正相关。在60 a尺度上,超前PDO负位相4 a和滞后AMO正位相12 a的高度场合成结果为AO负位相;在20～30 a尺度上,超前PDO正位相12 a和超前AMO正位相8 a的高度场合成结果为AO正位相。合成分析结果进一步验证了三个模态的相关性。 相似文献
6.
本文基于动力调整方法,利用客观分析海气通量（OAFlux）资料研究了1958～2016年全球海洋蒸发量变化及其动力作用和辐射强迫分量的变化,发现海洋蒸发量及其动力作用分量具有一致性年代际变化特征,特别是在20世纪70年代及90年代末期存在明显的年代际转折。进一步分析发现:主要动力因子有太平洋—北美遥相关型（PNA）、北极涛动（AO）、北大西洋涛动（NAO）、厄尔尼诺—南方涛动（ENSO）和阿留申低压（AL）,并受到太平洋年代际振荡（PDO）的影响,其中,1970年代末期的转折与PNA、PDO、ENSO和AL密切相关,而1990年代末期的转折还与NAO变化有关。动力作用分量的前六个模态解释方差达到67.5%,其中,低纬北太平洋和印度洋蒸发异常主要与海表温度（SST）及其引起的环流异常有关,南太平洋、中纬北太平洋和北大西洋蒸发异常与环流异常直接相关。ENSO与PDO在全球海洋蒸发量上的影响要大于NAO。单因子相关分析发现南方涛动指数（SOI）、NAO和PDO与海洋蒸发年代际变化密切相关。总体来说,动力作用分量在海洋蒸发的年代际变化中起主导作用,其中,以ENSO、NAO和PDO的影响最大。 相似文献
7.
热带和热带外太平洋海气相互作用特征的比较 总被引：2，自引：0，他引：2
比较分析了热带和热带外太平洋海气系统年际和年代际变化特征。在海气系统异常的方差构成中，北太平洋区域以年代际异常为主，热带太平洋区域年际和年代际异常相当；表（浅）层海洋与大气的年代际变化特征对同一季节、区域是一致的，且20世纪70年代后期到80年代初均发生由低模态向高模态的转变；北太平洋区域的7月与此不同，这与该季节近表层海温层结稳定有关；年际尺度的海、气异常与ENSO有关，且以热带太平洋区域1月最典型，7月次之，北太平洋区域1月再次之，7月无明显关系。 相似文献
8.
北太平洋阻塞的年际年代际变化及其与SST、遥相关及风暴路径的关系 总被引：2，自引：0，他引：2
利用NCEP／NCAR再分析资料，对1948／1949－1999／2000共52个冬季的北太平洋上空中纬度阻塞异常的气修特征进行了统计分析，小波分析和功率谱分析结果表明该区域阻塞发生的频数具有很明显的3－7年的年际振荡和年代际变化特征。同时2－7年带通平均的小波方差谱分析结果表明阻塞的这种年际变化的振幅存在着缓慢下降的趋势，且气候突变在20世纪70年代，这进一步证明了北太平洋上空的阻塞活动具有年代际变化特征。对强阻塞异常的冬季和弱阻塞异常的冬季分别进行合成分析，结果表明，对于阻塞异常强的冬季，北太平洋西向东北方向加强并分裂成两个中心，而SST异常在中纬度太平洋则对应着典型的PDO型，在赤道地区则为类La Nina型的海温分布。而对于阻塞异常弱的冬季则对应截然不同甚至相反的分布特征，即500hPa高度异常场表现为符号相反的PNA型，风暴路径中心在日界线附近呈纬向型分布。同时SST异常在赤道地区则为典型的El Nino型的海温分布。以上结果揭示出北太平洋阻塞活动的年际变化可能主要与热带海温的遥响应相联系，而年代际变化则主要与中纬度局地的PDO型海温及其通过斜压瞬变波的海－气相互作用有关。 相似文献
9.
近百年中国东部夏季降水年代际变化特征及其原因 总被引：15，自引：4，他引：11
本文利用测站降水观测资料分析过去一百多年中国东部华北、长江流域以及华南夏季降水的年代际变化特征发现,尽管这三个地区的夏季降水具有不同的年代际转折时期,但是均同时在1910年代初期、1920年代初期、1940年代中期、1960年代中期、1970年代末期以及1990年代初期发生了跃变。近一百年间不同年代际时期东部夏季降水的分布型主要以南正北负或者南负北正的偶极型为主,并且无论是偶极型分布还是三极型分布,两个相邻年代际时期中国东部降水分布型发生完全反向变化的概率较高（60%）。此外,夏季的PDO、冬季的AO以及春季的北极海冰也同时在1920年代末期、1940年代中期、1970年代末期以及1990年代中期左右发生了跃变,这几次跃变时期与中国东部三个不同地区夏季降水发生跃变的时期一致,表现出近百年来太平洋年代振荡（PDO）、北极涛动（AO）以及北极海冰这三个因子对中国东部夏季降水年代际变化的协同作用。在年代际时间尺度上,夏季的PDO与华北夏季降水显著负相关。PDO的年代际变化能够在500 hPa位势高度场中激发出太平洋—日本（PJ）型年代际遥相关波列;同时在850 hPa风场中激发出类似于影响华北夏季降水年代际变化的大气环流型,从而影响华北降水的年代际变化。冬半年的AO与长江流域夏季降水存在显著正相关关系。冬季到春季正位相的AO导致亚洲大陆南部处于湿冷状态,土壤湿度的记忆性可将这种状态延续到夏季。因此,夏季海陆热力对比减弱,东亚夏季风发生年代际减弱,相应地长江流域的降水年代际增多。春季北极海冰与华南夏季降水显著负相关,北极海冰的年代际异常能在500 hPa位势高度场中激发出与静止Rossby波异常传播相联系的欧亚—华南年代际遥相关波列,从而影响华南降水的年代际变化。 相似文献
10.
太平洋年代际振荡（PDO）是北太平洋海表温度年代际变率的主模态。由于太平洋年代际振荡对区域乃至全球气候的显著影响,其合理的预测结果可以带来多方面收益。然而,针对太平洋年代际振荡及其有关的海表温度的年代际预测,目前气候模式的预测水平还十分有限,因此,提出了一个新的增量方法。一系列的验证结果表明,增量方法可以有效预测太平洋年代际振荡,其中包括成功预测出其振荡的年代际转折。增量方法的预测过程主要包括3个步骤:（1）采用5 a滑动平均得到太平洋年代际振荡的年代际变率;（2）利用3 a增量形式的预测因子构建预测模型,预测3 a增量的太平洋年代际振荡（DI_PDO）;（3）将预测得到的DI_PDO加上3 a前的观测PDO,得到最后预测的PDO。增量方法亦可以应用到气候系统年代际内部变率的其他模态（如:北大西洋年代际振荡）和其他气候变量的年代际预测（如:海表温度）。 相似文献
11.
The Impact of Global Warming on the Pacific Decadal Oscillation and the Possible Mechanism简 总被引：1，自引：0，他引：1
The response of the Pacific Decadal Oscillation （PDO） to global warming according to the Fast Ocean Atmosphere Model （FOAM） and global warming comparison experiments of 11 IPCC AR4 models is investigated. The results show that North Pacific ocean decadal variability, its dominant mode （i.e., PDO）, and atmospheric decadal variability, have become weaker under global warming, but with PDO shifting to a higher frequency. The SST decadal variability reduction maximum is shown to be in the subpolar North Pacific Ocean and western North Pacific （PDO center）. The atmospheric decadal variability reduction maximum is over the PDO center. It was also found that oceanic baroclinic Rossby waves play a key role in PDO dynamics, especially those in the subpolar ocean. As the frequency of ocean buoyancy increases under a warmer climate, oceanic baroclinic Rossby waves become faster, and the increase in their speed ratio in the high latitudes is much larger than in the low latitudes. The faster baroclinic Rossby waves can cause the PDO to shift to a higher frequency, and North Pacific decadal variability and PDO to become weaker. 相似文献
12.
Climate Dynamics - Investigation into the Pacific decadal oscillation’s (PDO’s) role in modulating the intra-basin frequency of North Atlantic Rossby wave breaking (RWB) is carried out... 相似文献
13.
The response of the North Pacific Decadal Variability to strong tropical volcanic eruptions 总被引：5，自引：2，他引：3
In this study, the effects of volcanic forcing on North Pacific climate variability, on interannual to decadal time scales, are examined using climate model simulations covering the last 600?years. The model used is the Bergen Climate Model, a fully coupled atmosphere–ocean general circulation model. It is found that natural external forcings, such as tropical strong volcanic eruptions (SVEs) and variations in total solar irradiance, play an important role in regulating North Pacific Decadal Variability (NPDV). In response to tropical SVEs the lower stratospheric pole–to–equator temperature gradient is enhanced. The North polar vortex is strengthened, which forces a significant positive Arctic Oscillation. At the same time, dipole zonal wind anomalies associated with strong polar vortex propagate downward from the lower stratosphere. Through positive feedbacks in the troposphere, the surface westerly winds across the central North Pacific are significantly weakened, and positive sea level pressure anomalies are formed in the North Pacific. This anomalous surface circulation results in changes in the net heat fluxes and the oceanic advection across the North Pacific. As a result of this, warm water converges in the subtropical western North Pacific, where the surface waters in addition are heated by significantly reduced latent and sensible heat fluxes from the ocean. In the eastern and high–latitude North Pacific the ocean loses more heat, and large–scale decreases in sea surface temperatures are found. The overall response of this chain of events is that the North Pacific enters a negative phase of the Pacific decadal oscillation (PDO), and this negative phase of the PDO is maintained for several years. It is thus concluded that the volcanic forcing plays a key role in the phasing of the PDO. The model results furthermore highlight the important role of troposphere–stratosphere coupling, tropical–extratropical teleconnections and extratropical ocean–atmosphere interactions for describing NPDV. 相似文献
14.
This study utilizes a new monthly-assimilated sea temperature and analyzes trend and decadal oscillations in tropical Pacific 100-200 m subsurface ocean temperature (SOT) from 1945 to 2005 on the basis of the harmonic analysis and Empirical Orthogonal Function (EOF) methods. Significant cooling trends in the SOT in the tropical western Pacific were found over this 60-year period. The first EOF of the SOT in tropical Pacific displays an ENSO-like zonal dipole pattern on decadal time scale, and we considered this pattern in subsurface ocean temperature the tropical Pacific decadal oscillation (TPDO). Our analysis suggests that TPDO is closely correlated with the Pacific decadal oscillation (PDO) in the surface sea temperature (SST). The correlation coefficient between the indices of TPDO and PDO is +0.81 and reaches a maximum of +0.84 when TPDO lags behind PDO by 2 months. Therefore, a change of TPDO is likely related to the variation of PDO. The long-term change in TPDO best explains decadal warming in the tropical eastern Pacific SST and implies potential impact on the weakening of East Asian summer monsoons after the late 1970s. 相似文献
15.
北半球冬季阿留申低压－冰岛低压相关关系的年代际变化及其模拟 总被引：1，自引：0，他引：1
使用多种长期观测和再分析资料,分析了北半球冬季阿留申低压和冰岛低压相关关系的年代际变化。结果表明,两低压存在显著的负相关关系,使北太平洋和北大西洋海平面气压形成跷跷板式的变化(Aleutian Low-Icelandic Low Seesaw,AIS)。此外,AIS还存在显著的年代际变化,在1935~1949年和1980年后较为显著,其余时期并不显著。对1980年代的年代际转变分析表明,太平洋年代际振荡(Pacific Decadal Oscillation,PDO)在1970年代末的位相转变是AIS这次年代际转变的主要原因。PDO由负位相转变为正位相,使全球大部分大洋海表温度升高,而北太平洋海表温度降低,两低压显著变深,低压南部西风增强,从而通过Rossby波的频散效应使两低压强度形成显著负相关。1930年代中期的年代际转变与此类似,但强度较弱。同时,年代际背景的变化也影响到两低压的年际变化。在给定海表温度和海冰分布的驱动下,大气环流模式IAP AGCM4能基本模拟出AIS年代际转变的过程和机理,但仍存在一些偏差。 相似文献
16.
On the predictability of decadal changes in the North Pacific 总被引：2，自引：0，他引：2
The predictability of decadal changes in the North Pacific is investigated with an ocean general circulation model forced
by simplified and realistic atmospheric conditions. First, the model is forced by a spatially fixed wind stress anomaly pattern
characteristic for decadal North Pacific climate variations. The time evolution of the wind stress anomaly is chosen to be
sinusoidal, with a period of 20 years. In this experiment different physical processes are found to be important for the decadal
variations: baroclinic Rossby waves dominate the response. They move westward and lead to an adjustment of the subtropical
and subpolar gyre circulations in such a way that anomalous temperatures in the central North Pacific develop as a delayed
response to the preceding wind stress anomalies. This delayed response provides not only a negative feedback but also bears
the potential for long-term predictions of upper ocean temperature changes in the central North Pacific. It is shown by additional
experiments that once these Rossby waves have been excited, decadal changes of the upper ocean temperatures in the central
North Pacific evolve without any further anomalous atmospheric forcing. In the second part, the model is forced by surface
heat flux and wind stress observations for the period 1949–1993. It is shown that the same physical processes which were found
to be important in the simplified experiments also govern the evolution of the upper ocean in this more realistic simulation.
The 1976/77 cooling can be mainly attributed to anomalously strong horizontal advection due to the delayed response to persistent
wind stress curl anomalies in the early 1970s rather than local anomalous atmospheric forcing. This decadal change could have
been predicted some years in advance. The subsequent warming in the late 1980s, however, cannot be mainly explained by advection.
In this case, local anomalous atmospheric forcing needs to be considered.
Received: 6 July 1998 / Accepted: 16 October 1999 相似文献
17.
Mark R. Jury 《大气与海洋》2013,51(5):322-331
ABSTRACTSouth Indian Ocean Rossby waves (SIO-RW) are identified in the Global Ocean Data Assimilation System (GODAS) 1.5–7?yr filtered sea surface height (SSH) time series. There is a persistent three-year oscillation in the 5°–15°S latitude band from 55° to 85°E. Field correlations show little coupling at 90°E, but as the SIO-RW undulates westward at approximately 0.19?m?s?1 across the mid-basin, a northwest–southeast axis of warm sea surface temperatures (SSTs) and deep convection forms. Many teleconnections in earlier work are confirmed: interannual pulses of zonal wind in the eastern basin trigger the SIO-RW via anticyclonic wind stress curl. New insights derive from an understanding of links with the upper troposphere. As the SIO-RWs move westward with the onset of an El Niño in the Pacific, increased convection over the north Indian Ocean corresponds to reduced evaporation and SST warming. Mid-tropospheric heating T′?>?2°C over the northwest Indian Ocean accelerates the southern sub-tropical jet to greater than 10?m?s?1 over the southeast Indian Ocean, reinforcing the anticyclonic vorticity. The downstream acceleration of the jet generates upper-level divergence and moist convection over the western basin, anchoring an atmospheric Rossby wave in a northwest–southeast alignment underpinned by differential propagation of the SIO-RW. As the ocean Rossby wave reaches Africa, the coupling fades and transitions. What distinguishes Indian Ocean from Pacific Ocean Rossby waves are their southern latitude and higher frequency. The tropical mid-tropospheric heating that accelerates the southern sub-tropical jet shifts westward in tandem with the SIO-RW. 相似文献
18.
Jae-Heung Park Soon-Il An Sang-Wook Yeh Niklas Schneider 《Theoretical and Applied Climatology》2013,112(3-4):431-445
The Pacific decadal oscillation (PDO) is defined as the first empirical orthogonal function (EOF) mode of the North Pacific sea surface temperature anomalies. In this study, we reconstructed the PDO using the first-order autoregressive model from various climate indices representing the El Niño-Southern oscillation (ENSO), Aleutian Low (AL), sea surface height (SSH), and thermocline depth over the Kuroshio–Oyashio extension (KOE) region. The climate indices were obtained from observation and twentieth-century simulations of the eight coupled general circulation models (CGCMs) participating in the Climate Model Intercomparison Project Phase III (CMIP3). In this manner, we quantitatively assessed the major climate components generating the PDO using observation and models. Based on observations, the PDO pattern in the central to eastern North Pacific was accurately reconstructed by the AL and ENSO indices, and that in the western North Pacific was best reconstructed by the SSH and thermocline indices. In the CMIP3 CGCMs, the relative contribution of each component to the generation of the PDO varied greatly from model to model, and observations, although the PDO patterns from most of the models were similar to the pattern observed. In the models, the PDO pattern in the eastern and western North Pacific were well reconstructed using the AL and SSH indices, respectively. However, the PDO pattern reconstructed by the ENSO index was quite different from the observed pattern, which was possibly due to the model's common deficiency in simulating the amplitude and location of the ENSO. Furthermore, the differences in the contribution of the KOE thermocline index between the observed pattern and most of the models indicated that the PDO pattern associated with ocean wave dynamics is not properly simulated by most models. Therefore, the virtually well simulated PDO pattern by models is a result of physically inconsistent processes. 相似文献