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1.
热带和中高纬地区季节内振荡的特征及其动力学诊断   总被引:3,自引:0,他引:3  
使用5年低阶全球谱模式资料,对中高纬大气和热带大气季节内振荡的动力学性质和传播特征进行了诊断研究。分析发现模式再现了大气中季节内振荡在热带和中高纬地区的传播特性以及它们之间的差异。热带大气30—60天振荡在速度势场上表现为纬向—波结构和行波特性,而在散度风场上反映了赤道西太平洋—印度洋东西向偶极子型的振荡。中高纬大气30—60天振荡表现为定常波位相和振幅的变化,即波包络的传播特征。它与中高纬地区遥相关型的转换有关,通过遥相关位相和振幅的变化,不仅完成了热带和中高纬地区之间以及热带不同区域之间的能量输送,而且通过这种能量输送过程把南、北半球中高纬地区季节内振荡联系起来。   相似文献   

2.
热带大气中的准双周(10—20天)振荡   总被引:10,自引:3,他引:10  
李崇银  周亚萍 《大气科学》1995,19(4):435-444
基于欧洲中期天气预报中心(ECMWF)的资料(1981—1988),本文对全球热带大气中的10—20天(准双周)振荡进行了比较系统的研究,包括其动能的分布及演变。扰动的结构和传播特征等。资料分析充分表明,热带大气10—20天振荡是热带大气中另一重要低频系统,其动能比30—60天振荡还要大,而其结构和活动又同30—60天振荡很不一样。例如热带大气10—20天振荡主要表现为纬向波数2—4;垂直结构以正压特征更显著;主要表现为向西传播;其经向风分量与纬向风分量同等重要。因此,对热带大气10—20天振荡值得更多注  相似文献   

3.
An atmospheric general circulation model is used in a series of three experiments to simulate the intraseasonaloscillation in the tropical atmosphere.Analyses of the model daily data show that various physical variables,from sever-al different regions,exhibit fluctuations with a spectral peak between 30 and 60 days.This represents a 30—60 dayoscillation in the tropical atmosphere and possesses several features which are consistent with observations.These in-clude a horizontal structure dominated by zonal wavenumber 1 and a vertical structure which is predominantlybaroclinic.The effect of warm SST (sea surface temperature) anomalies on the 30—60 day oscillation in the tropical atmos-phere is also simulated by prescribing global SST as observed in 1983.This has the effect of weakening the oscillationwhile at the same time the vertical structure becomes less baroclinic.The importance of cumulus convection to the propagational characteristics of this oscillation is demonstrated by acomparison of results based on different parameterizations for convection.In one case,where the maximum convectionover the Pacific is simulated to be too far east,the simulated 30—60 day oscillation shows evidence of westward propa-gation.In the second case,where the convection maximum is located near the observed position in the western Pacific,there is more clearly evidence of eastward propagation.Both results suggest that the location of maximum convection in the Pacific can have an important influence on thestrength,structure and propagation of the 30—60 day oscillation.  相似文献   

4.
30—60天大气振荡的全球特征   总被引:14,自引:6,他引:14       下载免费PDF全文
李崇银 《大气科学》1991,15(3):66-76
利用ECMWF格点资料,分析研究了大气季节内(30—60天)振荡的全球特征。30—60天振荡动能的分布表明高纬度地区要比赤道地区大得多。说明那里有较突出的30—60天振荡。中高纬度地区的30—60天振荡与热带有明显不同,垂直结构为正压模态,以纬向2—4波为主,多为向酉传播。30—60天振荡存在明显的低频遥相关,北半球主要为欧亚—太平洋(EAP)型和PNA型,南半球主要有澳洲—南非(ASA)型和环南美(RSA)型,并且在全球范围构成南北半球相互衔接的低频波列,即EAP-ASA波列和PNA-RSA波列。南北半球30—60天大气振荡有明显的相互影响,本文研究了南北半球30—60天振荡相互影响的3种主要过程。  相似文献   

5.
In this paper, five-year simulated data from a low-resolution global spectral model with triangular trunca-lion at wavenumber 10 are analyzed in order to study dynamical features and propagation characteristics ofintraseasonal oxillations over the mid-latitudes and the tropical atmosphere. The simulations show that thereis the 30-50 day periodic oscillation in the low-resolution spectral model without non-seasonal external forcing,and spatial scale of the intraseasonal oscihations is of the globe .Further analysis finds that propagation charac-ters of intraseasonal oscillations over the mid-latitudes and the tropics are different. The 30-50 day oscillationover the tropics exhibits structure of the velocity potential wave with wavenumber 1 in the latitudinal and thecharacter of the traveling wave eastward at speed of 8 longitudes/day. However, the 30-50 day oscillationsin mid-latitude atmosphere exhibit phase and amplitude oscillation of the standing planetary waves and theyare related to transform of teleconnection patterns over the mid-latitudes. The energy is not only transferredbetween the tropics and the middle-high latitudes, but also between different regions over the tropics. Based on the analysis of 5-year band pass filtered data from a 5-layer global spectral model of Jow-ordetwith truncated wavenumber l0,investigation is done of the source of intraseasonal oscillations in the extratropicalmodel atmosphere and its mechanism. Results show that (1) the convective heat transferred eastward alongthe equator serves as the source of the intraseasonal oxillation both in the tropical and the extratropical atmos--phere; (2) the velocity-potential wave of a zonal structure of wavenumber 1 gives rise to oxillation in divergentand convergent wind fields of a dipole-form as seen from the equatorial Indian Ocean to the western Pacificduring its eastward propagation, thus indicating the oscillation in the dipole-form heat soure:e/sink pattertl; (3)the tropical heat-source oscillation is responsible for the variation in phase and intensity of the extratropicalstationary wave train, and the interaction between the oscillating low-frequency inertial gravity and stationaryRossby modes that are probably mechanisms for the oscillations ip the middle-high latitudes.  相似文献   

6.
夏季风场40—50天振荡的全球分布及波动特征   总被引:1,自引:0,他引:1  
  相似文献   

7.
本文用1980年5—9月ECMWF客观分析资料,对青藏高原上空30—60天振荡进行研究。结果表明,与高原附近30—60天振荡相联系的遥相关波列有两支,一支为高原-伊尔库茨克-欧洲-大西洋东部;另一支为青藏高原-伊尔库茨克-雅库茨克-堪察加半岛-阿留申群岛。30—60天振荡在高原北侧和南侧地区,对流层上层和下层表现出不同的垂直结构。时间变化主要表现为向西的能量频散。  相似文献   

8.
运用IAPAGCM模式证实了大气对南极冰异常的强迫遥响应是激发产生全球大气季节内振荡的重要机制,进而着重考察了候平均偏差结果的时间序列,并且通过带通滤波处理,特别分析了响应场中30~60d低频振荡的特征及其活动。通过分析发现:大气对南极冰减退的响应是一种具有30~60d周期的低频遥响应,并呈现出清楚的二维Rossby波列特征;强迫场中的30~60d季节内振荡具有着同实际大气中的低频振荡相类似的垂直结构和传播特征。大气响应场中30~60d振荡能量在垂直方向上随高度的增加而增加,在纬向上表现出明显的区域性特征,即季节内振荡的最大动能区(由于CISK机制)分布在大洋内;EUP,PNA,ASA和RSA波列可能是全球大气低频扰动传播的主要路径,30~60d低频扰动在波列路径上的传播具有很大的一致性和系统性,从而使中高纬和热带地区、以及南北半球的30~60d大气振荡相互联系起来,而且可以认为,赤道中太平洋和赤道中大西洋地区是南北半球30~60d低频振荡间相互作用和相互联系的重要通道。  相似文献   

9.
该文利用冬季500 hPa的欧洲中心(ECMWF)网格点逐日资料,分析了30—50天振荡的E矢量分布、动能特性及平均气流的正压不稳定能转换特征,从而得到:30—50天振荡的能量传播与西风急流的位置有密切的关系,在西风大风速区作纬向能量传播,在小风速区作指向赤道的经向传播;在急流的出口区有较强的正压能转换,低频振荡从基本流中获得能量,使这里的低频动能最大,并表现出较强的正压特性,与低纬度的斜压特性形成鲜明对照。  相似文献   

10.
本文应用中央气象局出版的“北半球高空气候图集”中的风场资料,计算了45°N以南、北半球范围、7月份850 mb—100 mb各标准等压面层上的平均垂直运动。分析了不同区域经向和纬向垂直环流的特点,并将它与大气中冷热源进行对照。指出:夏季北半球低纬度平均是个Hadley环流,其北是个道环流。形成这种环流形势的主要贡献地区在两个大洋上,这主要与低纬度大气是个热源、共北是个冷源的分布有关。另外,由纬向环流看到,夏季北半球中低纬主要上升运动区和下沉运动区各有两个,这两对上升气流区和下沉气流区构成了夏季北半球中低纬地区垂直环流的大形势。此外,本文还指出夏季青藏高原上空的上升气流向四周流出后所影响的地理区域。  相似文献   

11.
热带大气季节内振荡的一个数值模拟研究   总被引:9,自引:2,他引:9  
文中分析了中国科学院大气物理研究所全球气候谱模式ALGCM (R4 2L9) 12a(1978~ 1989年 )积分的逐日输出结果 ,并与 1978~ 1989年的逐日NCEP资料对照 ,以此对热带季节内振荡 (30~ 6 0d振荡 )进行数值模拟研究。分析表明 ,该模式在热带地区可以模拟出明显的季节内振荡 (ISO)的准周期信号 ,并抓住了热带ISO的基本传播特征 ,能较好地再现东、西半球传播速度的差异 ,同时模式模拟存在东传要好于西传 ,冬、春季的模拟要好于夏、秋季的现象。该模式模拟的热带ISO的强度较许多大气模式明显提高 ,尤其是对 2 0 0hPa上ISO动能强度的模拟。模式基本模拟出了ISO低层辐合、高层辐散的水平风场特征。模式较好地再现了热带ISO纬向风的垂直结构。此外 ,观测资料表明热带ISO在冬、春强 ,而夏、秋弱的季节性倾向与ISO的年际变化相联系 ,模拟的ISO在季节性倾向偏差上表现为冬、夏相对强 ,而春、秋相对弱。垂直速度、散度、水汽等物理量的配置同NCEP资料的结构特征仍有明显差异 ,模拟的ISO空间分布也不太理想 ,表明要很好模拟ISO结构和空间分布特征 ,还须做不少工作。  相似文献   

12.
东亚梅雨季节内振荡的气候特征   总被引:7,自引:1,他引:6  
梁萍  丁一汇 《气象学报》2012,70(3):418-435
影响中国、日本、朝鲜半岛的东亚梅雨是夏季风向北推进过程中的特有雨季。利用NCEP/NCAR逐日再分析资料、CMAP降水资料,将夏季风影响及夏季风降水的季节转换相结合,定义东亚梅雨的入、出梅指标;进而采用集合经验模态分解信号提取方法对东亚梅雨区降水季节内振荡及其大尺度环流条件的气候特征进行了详细分析;并对东亚梅雨季节内振荡对降水事件的指示作用进行讨论,为东亚梅雨区降水的延伸预报提供依据和参考。研究结果表明:(1)采用标准化候降水量的空间覆盖率,同时兼顾夏季风影响等条件确定的东亚梅雨入、出梅划分指标可较好地反映东亚梅雨的气候特征及东亚梅雨期的大尺度环流形势。(2)东亚梅雨全年降水量存在三峰型分布特征,峰值分别位于第27、36及47候。该三峰型特征主要受10—20及30—60d的低频振荡影响。比较而言,30—60d振荡对梅雨区降水三峰型的贡献较10—20d振荡大。(3)东亚梅雨区峰值降水与热带环流及北方高位涡冷空气输送的低频演变密切关联。在梅雨区北侧,中高纬度里海附近冷空气(高位涡)低频波列的东传及鄂霍次克海高位涡的西南向输送共同影响东亚梅雨区。在梅雨区南侧,通过热带低频异常强对流的激发作用,热带西太平洋至中国东北—鄂霍次克海地区形成沿经向分布的低层气旋-反气旋-气旋-反气旋波列,进而导致梅雨区低层形成低频偏北风和偏南风的辐合;而印度西海岸和阿拉伯海地区异常对流活动产生的波列向东北方向传播,亦对梅雨区低频峰值降水产生影响。对于低频谷值降水的大气低频演变,情况与上述基本相反。(4)东亚梅雨区降水不同位相下出现极端降水事件的概率有明显差异。梅雨区降水低频峰(谷)值位相下出现异常多(少)降水量的概率约为30%。因此,上述梅雨区降水低频振荡演变相关的大气低频振荡特征对梅雨区降水事件的延伸预报具有参考价值。  相似文献   

13.
Based on the NCEP/NCAR reanalysis data and the observed precipitation data in the south of China from 1958 to 2000,the impact of 30 to 60 day oscillation of atmospheric heat sources on the drought and flood events in June in the south of China is discussed.During the flood(drought) events,there exists an anomalous low-frequency anticyclone(cyclone) at the low level of the troposphere over the South China Sea and the northwestern Pacific,accompanied with anomalous low-frequency heat sinks(heat sources),while there exists an anomalous low-frequency cyclone(anticyclone) with anomalous heat sources(sinks) over the area from the south of China to the south of Japan.On average,the phase evolution of the low-frequency in drought events is 7 to 11 days ahead of that in flood events in May to June in the south of China.In flood events,low-frequency heat sources and cyclones are propagated northward from the southern South China Sea,northwestward from the warm pool of the western Pacific and westward from the northwestern Pacific around 140°E,which have very important impact on the abundant rainfall in June in the south of China.However,in drought events,the northward propagations of the low-frequency heat sources and cyclones from the South China Sea and its vicinity are rather late compared with those in flood events,and there is no obvious westward propagation of the heat sources from the northwestern Pacific.The timing of the low-frequency heat source propagation has remarkable impact on the June rainfall in the south of China.  相似文献   

14.
Temporal and spatial evolution characteristics of the 30-60 day oscillation (intraseasonal oscillation, ISO) of summer rainfall in China and the effects of East Asian monsoon on the rainfall ISO are analyzed in this paper. Results show that the annual and decadal variations of the oscillation exist between 1960 and 2008, and the intensity is weakest in the late 1970s and early 1980s. In the typical strong years of the rainfall ISO obtained from empirical orthogonal functions (EOF mode 1), an anticyclone is in northwestern Pacific and a cyclone is in the east of China. In the typical weak years, the wind ISO is much weaker. The low-frequency zonal wind and water vapor transport from the low latitudes to mid-latitudes in the typical strong years, and the oscillation strength of diabatic heating is much stronger than that in the weak years of the rainfall ISO. The anomaly characteristics of the rainfall ISO show anti-phases between the Yangtze River basin and south of China. As for the typical strong years of the rainfall ISO in the Yangtze River basin (EOF mode 2), the main oscillation center of water vapor is in the east of China (20-30°N, 110-130°E). In the peak (break) phase of the rainfall oscillation, a low-frequency cyclone (anticyclone) is in the Yangtze River basin and an anticyclone (cyclone) is near Taiwan Island. In addition, the peak rainfall corresponds to the heat source in the Yangtze River basin and the heat sink in the Qinghai-Tibet Plateau. As for the typical strong years of the rainfall ISO in the south of China, the main oscillation center of water vapor is south of 20°N. In the peak (break) phase of the rainfall ISO, a low-frequency cyclone (anticyclone) is in the south of China and an anticyclone (cyclone) is in the Philippines. The peak rainfall corresponds to the heat source in the south of China and the South China Sea, and the heat sink in the west of Indochina.  相似文献   

15.
登陆台风与其外围暴雨的相互作用   总被引:13,自引:4,他引:13  
励申申  寿绍文  王信 《气象学报》1992,50(1):33-40,49
本文对8116号登陆台风及其环境和外围暴雨区分别作了动能平衡的诊断分析,结果表明,动能制造是三个区域动能平衡的主要能源,动能水平辐散和摩擦消耗则是主要能汇。在台风登陆减弱过程中,暴雨区的动能增加。台风区上层动能水平辐散呈显著的不对称型。台风右侧次天气尺度强风带起了向暴雨区输送动能使暴雨得到发展的作用。暴雨发生后,通过暴雨区北界向环境输送动能,于是,台风辐散的动能通过暴雨区最后输送给环境。这种动能传递过程可能是台风与环境大气相互作用引起台风衰减的机制之一。  相似文献   

16.
IAP-GCM is used to document the forced teleresponse of the atmosphere to anomalies of the Antarctic sea ice as the important triggering mechanism for intraseasonal atmospheric oscillations across the globe. The time series of pentad-averaged deviations are then focused on and. with the band-pass filter approach, to address essential features of the 30-60 day low-frequency oscillation in the response field. It is found that tile atmospheric response to the retreat of the Antarctic sea ice is of low frequency at a period of 30-60 days. The main component is the 30-60 day intraseasonal oscillation in the forced field, with the vertical structure and distribution features similar to real atmosphere.  相似文献   

17.
利用高分辨率(10km)数值模拟的结果,以登陆华南并引发特大暴雨的0601号台风为例,对台风中田尺度动能收支平衡进行了诊断分析。结果表明,中-β尺度系统动能收支水平项(水平通量散度项和水平产生项)很小,垂直项(垂直通量散度项和垂直产生项)是动能收支方程的主要部分;动能垂直通量散度在对流层低层是动能的汇,在对流层中高层为动能的源;动能垂直产生项在对流层各层都是动能的汇;浮力产生项在300hPa以下是动能的源,在对流层高层是动能的汇;平均动能的局地变化项,在对流层各层均小于零,暴雨期间对流层动能支大于收,且动能变化在对流层中低层最明显。就整个对流层的垂直总量而言,浮力产生项是主要的动能源,而垂直产生项是主要的动能汇。较强冷空气首先从对流层中层入侵台风环流系统,抑制动能制造和传输,是中田尺度对流系统不能维持、发展的主要原因,也是台风系统及其暴雨不能长久维持的关键。  相似文献   

18.
运用LAPGCM模式证实了大气对南极冰异常的强迫遥响应是激发全球大气季节内振荡的重要机制,进而着重考察候平均偏差结果的时间序列,并且通过带通以处理,特别分析了响应场中30-60天低频振荡的重要特征,发现:大报对南极冰减退的响应是一种具有30-60天周期的低频遥响应。强迫场中的重要成分是30-60天季节内振荡,并且具有同实际大气中的低频振荡相类的垂直结构以及传播和分布特征。  相似文献   

19.
许乐心  张人禾  齐艳军 《大气科学》2017,41(6):1125-1140
利用1979~2013年中国站点逐日降水资料和NCEP/NCAR再分析资料,对长江中下游夏季降水的季节内振荡最显著周期进行了分析研究。结果表明长江中游最显著周期为10~30天,长江下游最显著周期为30~60天。为了揭示这种差异产生的物理原因,进一步利用位相合成的方法对这两个区域不同周期的季节内振荡降水、高低空风场和高度场以及垂直结构和水汽等循环过程的演变特征进行分析。在200 hPa环流场上,长江中游的降水主要受到高纬度自西向东传播的波列影响,而长江下游的降水与鄂霍次克海的高度场的变化相关。在风场的垂直涡度和散度的位相结构演变过程中,10~30天的垂直涡度和散度有自北向南的移动,30~60天的垂直涡度和散度在长江以南地区有自南向北的传播。水汽输送的位相发展过程表明,长江中游的水汽分别来自于南海的向北输送和长江以北地区向南的水汽输送;长江下游地区的水汽则主要来自于热带东印度洋经孟加拉湾的向东输送并在南海的北向输送,以及西太平洋水汽向西输送到南海再向长江下游的输送。从高层大尺度环流场和整层积分的水汽通量输送上解释了长江中游10~30天降水的自北向南移动,和长江下游30~60天降水自南向北传播的原因。  相似文献   

20.
本文用热力学方程和水汽连续方程计算了东南亚地区1981年初夏的大气热源和水汽汇的分布情况。文章讨论了大气热源的演变与该地区经向垂直环流的相互关系,并讨论了大气热源和经向环流在南海和中南半岛的差异。分析结果表明,经向环流圈与大气冷热源的分布密切相关。东亚季风建立后的大气热源中心在南海北部,热汇区在赤道附近,相应的最大上升气流也出现在南海下沉区主要在赤道南侧,而且南海的经向环流比中南半岛的要强盛的多。大气热源对于经向环流圈的形成和维持有很大的作用。   相似文献   

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