共查询到18条相似文献，搜索用时 105 毫秒
1.
IAP AGCM4.0模式对热带大气季节内振荡的模拟评估 总被引：1，自引：1，他引：0
基于中国科学院大气物理所大气环流模式IAP AGCM4.0总共30年(1979~2008年)的模拟结果,评估了IAP AGCM4.0模式对热带大气季节内振荡的模拟能力。分析结果表明IAP AGCM4.0模式可以在一定程度上模拟出热带大气季节内振荡的主要时空谱结构特征,在周期30~80天处存在明显的谱能量中心;模式模拟的季节内振荡东传的主要特征与观测基本一致,东移波的能量远大于西移波。基于RMM指数(All-season Real-time Multivariate MJO Index)的分析表明,模式模拟的850 h Pa和200 h Pa季节内尺度风场和对流活动在赤道地区的空间分布与观测基本一致。但与观测相比,模式模拟的热带大气季节内振荡的周期较短,东传速度快于观测,虚假的西传特征过强,对流活跃区域范围较小、强度较弱。就非绝热加热而言,模式模拟结果与再分析资料比较接近,但最大加热在印度洋和西太平洋地区出现的位相较晚。进一步分析表明,模式中影响对流触发的相对湿度阈值(RHc)的不同取值(RHc分别取为85%、90%、95%和100%),可以显著影响热带大气非绝热加热垂直廓线,从而影响模式对热带大气季节内振荡的模拟;当对流触发相对湿度阈值取为90%时,IAP AGCM4.0模式对热带大气季节内振荡模拟的能力相对最好,非绝热加热垂直廓线在不同位相的分布特征也与再分析资料最为接近。这说明模式对流参数化方案中不同参数的合适选取,可以改进模式对热带大气季节内振荡的模拟能力。 相似文献
2.
外强迫对热带季节内振荡影响的模拟研究 总被引：3，自引：2，他引：3
应用经过修改的NCAR CCM3模式和CAM2模式进行的数值实验结果以及NCEP的GFS模式的输出结果讨论了海温等外强迫作用对热带季节内振荡的影响.结果表明,热带季节内振荡是热带大气固有的内部变率.它是由大气内部过程的相互作用决定的.但外强迫对热带季节内振荡的强度、传播方向等有明显的影响.当外强迫没有变化时,模式可以模拟出与观测近似的低频振荡.当作为外强迫的海温和太阳辐射有年内季节变化时,模式模拟的季节内振荡则明显减弱.当海温与辐射不仅有季节变化而且有年际变化时,模式模拟的季节内振荡会进一步减弱.具有长周期的外强迫还会削弱季节内振荡中东移波动的能量而增加静止波的强度.在与海洋模式耦合的状态下,模式不受来自海洋的外强迫影响,而是与海洋构成一个耦合系统,可以产生最强的季节内振荡. 相似文献
3.
基于1979—2000年的NCEP/NCAR海平面气压和位势高度场资料分析了南半球大气环流的准半年振荡 (半年波) 现象。结果表明:这一现象主要出现在南半球对流层低层的中高纬度和中高层的热带地区。对南半球热带外大气而言, 40°S和65°S是低层大气环流准半年振荡最为显著的两个纬度带, 半年波的贡献都超过了70%, 低层南半球中高纬度海平面气压场季节变化的反位相也主要体现为各自半年波分量变化的反位相。在此基础上, 检验了IAP 9L AGCM (大气物理研究所9层大气环流模式) 对这一现象模拟的能力, 模拟结果显示, 模式成功模拟了65°S处海平面气压场的准半年振荡现象, 其振幅略低于观测结果, 但模式对40°S处气压场准半年振荡的模拟效果较差。 相似文献
4.
大气季节内振荡的数值模拟比较研究 总被引：13，自引：0，他引：13
用国内外两个较好的大气环流模式、在观测海表温度的强迫下进行了长时间(1978—1989年)的数值积分,然后对数值模拟结果与NCAR/NCEP再分析资料进行比较分析,其结果清楚表明,模式模拟结果的均方根误差中有30%—40%是来自于模拟的大气季节内振荡的均方根误差。尤其是,大气季节内振荡模拟的均方根误差的分布形势与总的均方根误差的分布形势几乎完全一致。对热带地区大气季节内振荡动能的模拟结果与NCAR/NCEP再分析资料的比较分析表明,其差异也十分明显,说明模式对热带大气季节内振荡的模拟能力也还比较差。因此可以认为,大气季节内振荡在天气气候模拟中极为重要,而如何在数值模式中模拟好大气季节内振荡还需要进行很好地研究。 相似文献
5.
热带大气10～20天振荡的大气环流模式数值模拟 总被引：5，自引：0，他引：5
利用大气环流模式对热带大气10～20天振荡进行了数值模拟研究，其结果同观测资料分析基本一致。模式资料的功率谱及动能的分析表明，10～20天振荡确实比30～60天振荡更突出地存在于热带大气中。同热带大气30～60天振荡的结构有些不同，对于在热带10～20天振荡，除纬向1波外，纬向2波也很明显；流动的斜压结构特征欠佳；系统以较快速度沿赤道西移。暖SST事件对热带大气10～20天振荡的影响也进行了模拟，对结果的比较分析表明，暖STT将使10～20天大气振荡减弱，使其结构更趋正压性。 相似文献
6.
有关全球变暖对热带大气季节内振荡特征的影响及其数值模拟的研究 总被引：9，自引：6，他引：9
首先用资料诊断分析了全球变暖前后,热带大气低频振荡特征变化。研究发现,全球变暖前后,热带低频振荡的强度、分布、传播及周期等发生了一系列变化:ISO活跃区及强度范围均有不同程度的增大,气候变暖有缩小ISO强度季节差异趋势;气候变暖后,纬向东传波的大气季节内振荡能量增加,而西传波的能量相对减少;偏暖阶段,ISO振荡主周期相对分散,特别是较长周期的小波能量明显增大。然后利用动力学分析及数值模拟进一步探讨了热带低频振荡与海温的联系,对热带ISO的数值模拟进一步发现,大气模式与海洋模式耦合时,所模拟的热带季节内振荡较强;热带低频振荡的变化可能与全球变暖后海温场发生的变化有关。 相似文献
7.
热带大气季节内振荡的进一步分析 总被引：2，自引：1，他引：1
利用ＥＣＭＷＦ的格点资料对热带大气季节内振荡作了进一步分析研究,表明热带大气季节内振荡既有Ｋｅｌｖｉｎ波型扰动,也有Ｒｏｓｓｂｙ波型扰动;影响热带大气季节内振荡移动的主要因素有扰动波型和积云对流活动的异常;伴随ＥｌＮｉｎｏ事件的发生,热带大气季节内振荡的动能急剧减小,而准定常扰动动能急剧增大,既反映了热带大气季节内振荡对ＥｌＮｉｎｏ的激发作用,也说明了在ＥｌＮｉｎｏ期间热带大气季节内振荡偏弱的原因。 相似文献
8.
中国热带大气季节内振荡研究进展 总被引：7，自引：1，他引：6
热带大气季节内振荡(包括MJO)是大气环流的重要系统,它的活动及异常既对其他系统有一定的作用,也对长期天气和短期气候有明显影响。因此,热带大气季节内振荡一直是大气科学的前沿研究课题之一。文中对近5—10年中国学者的有关研究工作及其进展做了简要回顾和综合,主要包括:(1)热带大气季节内振荡特别是MJO的动力学机制;(2)热带大气季节内振荡以及MJO的数值模拟问题,特别是大气非绝热加热廓线对模式模拟MJO的重要作用;(3)热带大气季节内振荡和MJO,特别是在赤道西太平洋地区,与ENSO的相互作用关系;(4)热带大气季节内振荡(包括MJO)及其流场形势对西太平洋台风活动的重要影响,即MJO对西北太平洋台风生成数的调制作用,以及热带大气季节内低频气旋性(LFC)和反气旋性(LFAC)流场对西太平洋台风路径的影响;(5)热带大气季节内振荡(包括MJO)的活动及异常对东亚和南亚夏季风建立、活动异常的影响,以及它们与中国降水异常的密切关系。 相似文献
9.
热带太平洋海表温度年际变化对降水季节内振荡的影响 总被引：6，自引：0，他引：6
根据 １９８２—１９９２年期间的日平均 ＭＳＵ（Ｓｐｅｎｃｅｒ, １９９３）海洋降水和 ５天平均的ＣＭＡＰ（Ｘｉｅ＆ Ａｒｋｉｎ, １９９７）降水观测资料,分析了热带太平洋大气季节内振荡（ＭＪＯ）的年际变化特征。在太平洋海表温度（ＳＳＴ）年际变化的正常年份（１９８２—８３年, １９８６—８８年, １９９１—９２年）,均有明显的ＭＪＯ信号传到日界线以东并在中、东太平洋维持数月。热带ＭＪＯ活动强度的年际变化与局地ＳＳＴ的变化存在正相关。中、东太平洋降水的季节内振荡的年际变化与热带太平洋ＳＳＴ的最强正相关在Ｎｉｎｏ３区附近。以观测ＳＳＴ场强迫ＣＣＭ３大气模式的数值试验基本上真实地再现了１１年期间热带太平洋降水季节内振荡的年际变化总趋势,但模拟季节内振荡的强度较观测平均偏弱。对比分别采用周平均和月平均ＳＳＴ强迫场的积分结果,发现在中、东太平洋,二个积分模拟的降水季节内振荡强度的年际变化接近并且趋势与观测基本一致,而在西太平洋二个积分的模拟结果差别较大。这表明在热带中、东太平洋,ＳＳＴ强迫的年际变化对ＭＪＯ强度的变化有强的制约。而在ＭＪＯ总体活跃的热带西太平洋,ＳＳＴ强迫场的季节变化对模拟ＭＪＯ活动也有较大影响。ＣＣＭ３模拟 相似文献
10.
两个大气环流模式SAMIL和BCC_AGCM对北半球冬季极涡振荡的模拟对比 总被引：1，自引：1，他引：1
基于与NCEP再分析资料的比较, 本文利用大气环流模式SAMIL和北京气候中心大气环流模式BCC_AGCM的1950～1999年的AMIP试验模拟数据, 对北半球冬季环流及平流层极涡振荡的模拟性能进行了评估分析。结果表明两个模式都可以再现北半球环流基本型以及环流振荡的主导模态。对冬季气候平均态的模拟, 两个模式模拟的热带—热带外温度梯度均偏大, 极夜急流偏强, 极涡偏冷偏强;100～20 hPa平均位势高度场谐波分析表明两个模式模 拟的行星波偏弱;气候平均的10 hPa极夜急流均存在1个月的季节漂移, 200 hPa副热带西风急流较NCEP偏弱。两个模式模拟的环流变化的主导模态均代表极涡振荡, SAMIL极涡振荡的强度大于BCC_AGCM, BCC_AGCM极涡振荡的频率要高于SAMIL。连续功率谱分析表明, NCEP资料中极涡振荡存在4.6个月的显著周期, 相应地, SAMIL中为5.5个月的显著周期, BCC_AGCM中为4.8个月。NCEP资料中的极涡振荡主要发生在12～3月, SAMIL模拟的极涡振荡主要发生在2～3月, BCC_AGCM模拟的极涡振荡主要发生在2～4月。 相似文献
11.
Simulations of the Tropical Intraseasonal Oscillation by the Atmospheric General Circulation Model of the Beijing Climate Center 总被引：1，自引：0，他引：1 
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下载免费PDF全文 The performance of BCC (Beijing Climate Center) AGCM 2.0.1 (Atmospheric General Circulation Model version 2.0.1) in simulating the tropical intraseasonal oscillation (TIO) is examined in this paper.The simulations are validated against observation and compared with the NCAR CAM3 (Community Atmosphere Model version 3) results.The BCC AGCM2.0.1 is developed based on the original BCC AGCM (version 1) and NCAR CAM3.New reference atmosphere and reference pressure are introduced into the model.Therefore,the origi... 相似文献
12.
Intraseasonal oscillations in 15 atmospheric general circulation models: results from an AMIP diagnostic subproject 总被引：16，自引：1，他引：16
J. M. Slingo K. R. Sperber J. S. Boyle J.-P. Ceron M. Dix B. Dugas W. Ebisuzaki J. Fyfe D. Gregory J.-F. Gueremy J. Hack A. Harzallah P. Inness A. Kitoh W. K.-M. Lau B. McAvaney R. Madden A. Matthews T. N. Palmer C.-K. Parkas D. Randall N. Renno 《Climate Dynamics》1996,12(5):325-357
13.
The Beijing Climate Center atmospheric general circulation model: description and its performance for the present-day climate 总被引：15，自引：0，他引：15
Tongwen Wu Rucong Yu Fang Zhang Zaizhi Wang Min Dong Lanning Wang Xia Jin Deliang Chen Laurent Li 《Climate Dynamics》2010,34(1):149-150
The Beijing Climate Center atmospheric general circulation model version 2.0.1 (BCC_AGCM2.0.1) is described and its performance
in simulating the present-day climate is assessed. BCC_AGCM2.0.1 originates from the community atmospheric model version 3
(CAM3) developed by the National Center for Atmospheric Research (NCAR). The dynamics in BCC_AGCM2.0.1 is, however, substantially
different from the Eulerian spectral formulation of the dynamical equations in CAM3, and several new physical parameterizations
have replaced the corresponding original ones. The major modification of the model physics in BCC_AGCM2.0.1 includes a new
convection scheme, a dry adiabatic adjustment scheme in which potential temperature is conserved, a modified scheme to calculate
the sensible heat and moisture fluxes over the open ocean which takes into account the effect of ocean waves on the latent
and sensible heat fluxes, and an empirical equation to compute the snow cover fraction. Specially, the new convection scheme
in BCC_AGCM2.0.1, which is generated from the Zhang and McFarlane’s scheme but modified, is tested to have significant improvement
in tropical maximum but also the subtropical minimum precipitation, and the modified scheme for turbulent fluxes are validated
using EPIC2001 in situ observations and show a large improvement than its original scheme in CAM3. BCC_AGCM2.0.1 is forced
by observed monthly varying sea surface temperatures and sea ice concentrations during 1949–2000. The model climatology is
compiled for the period 1971–2000 and compared with the ERA-40 reanalysis products. The model performance is evaluated in
terms of energy budgets, precipitation, sea level pressure, air temperature, geopotential height, and atmospheric circulation,
as well as their seasonal variations. Results show that BCC_AGCM2.0.1 reproduces fairly well the present-day climate. The
combined effect of the new dynamical core and the updated physical parameterizations in BCC_AGCM2.0.1 leads to an overall
improvement, compared to the original CAM3. 相似文献
14.
Ravi P. Shukla 《大气与海洋》2014,52(4):321-330
In this study, we examine the characteristics of the boreal summer monsoon intraseasonal oscillation (BSISO) using the second version of the Climate Forecast System (CFSv2) and revisit the role of air–sea coupling in BSISO simulations. In particular, simulations of the BSISO in two carefully designed model experiments are compared: a fully coupled run and an uncoupled atmospheric general circulation model (AGCM) run with prescribed sea surface temperatures (SSTs). In these experiments an identical AGCM is used, and the daily mean SSTs from the coupled run are prescribed as a boundary condition in the AGCM run. Comparisons indicate that air–sea coupling plays an important role in realistically simulating the BSISO in CFSv2. Compared with the AGCM run, the coupled run not only simulates the spatial distributions of intraseasonal rainfall variations better but also shows more realistic spectral peaks and northward and eastward propagation features of the BSISO over India and the western Pacific. This study indicates that including an air–sea feedback mechanism may have the potential to improve the realism of the mean flow and intraseasonal variability in the Indian and western Pacific monsoon region. 相似文献
15.
The ability of AGCM to simulate the tropical intraseasonal oscillation (ISO) has been studied using the output of global spectral model (ALGCM (R42L9)) of the Institute of Atmospheric Physics, Chinese Academy of Sciences, and the outoput is compared with the results from NCEP/NCAR reanalysis for the year 1978-1989. The model displays an evident periodic signal of the tropical ISO. Basic propagating characters of the tropical ISO are captured, and changes in phase speed between Eastern and Western Hemispheres are also well presented, and the simulation of eastward propagation is better than that of westward propagation. This model has increased the ability to simulate the strength of the tropical ISO, especially at 200 hPa, and basically simulates the horizontal structure of wind characterized by the convergence in low-level and divergence in upper-level. The vertical structure of the zonal wind is also well reproduced. Moreover, observed results show that the representing of seasonal preference to form strong ISO in winter and spring is related to ISO's interannual variability, but it is shown in this model with strong ISO in winter and summer and weak ISO in spring and autumn. Structures of some physical elements such as vertical velocity, divergence, specific humidity, etc., and the special distribution of ISO have also differences with these from NCEP reanalysis data, which make it clear to develop this model to simulate the structure and spatial distribution of the ISO. 相似文献
16.
热带季节内振荡时空特征的诊断研究 总被引：24，自引：4，他引：24
文中应用谱分析、小波分析等方法及较长时段的资料进一步总结了热带季节内振荡的一些基本气候特征。热带季节内振荡主要活跃在 3个地区 ,最强的是西太平洋地区 ,其次是印度洋地区 ,第三是东太平洋沿岸的赤道以北地区。热带季节内振荡有明显的季节变化 ,西太平洋地区和印度洋地区的季节内振荡 1a中有两次极大值 ,冬季主要活跃在南半球 (10°S附近 ) ,而夏季则活跃在北半球 (10°N附近 ) ,春、秋季热带季节内振荡则明显减弱。东赤道太平洋北侧的季节内振荡只在夏季活跃 ,而冬季则很弱 ,且不随季节而南北移动。对于大气的大尺度要素 ,例如u风场 ,热带季节内振荡的能量主要集中在 1波。而对于像降水这样尺度较小的要素 ,热带季节内振荡的能量则相对较分散 ,尽管它仍然在 1波有最大的能量 ,但 2～ 4波也具有较接近的能量。热带季节内振荡以东移的波动为主。热带季节内振荡存在着年际甚至更长时间的变化。 2 0世纪 70年代末期季节内振荡的幅度有一明显的突变。 相似文献
17.
Xiaolong Jia Chongyin Li Ningfang Zhou Jian Ling 《Dynamics of Atmospheres and Oceans》2010,49(2-3):141-163
The Madden–Julian oscillation (MJO) is simulated using an AGCM with three different cumulus parameterization schemes: a moist convective adjustment (MCA) scheme, the Zhang–McFarlane (ZM) mass-flux scheme, and the Tiedtke scheme. Results show that the simulated MJO is highly dependent on the cumulus parameterization used. Among the three cumulus parameterizations, only the MCA scheme produces MJO features similar to observations, including the reasonable spatial distribution, intraseasonal time scales and eastward propagation. Meanwhile, the amplitude is too large and the eastward propagation speed too fast than observations and the relationship between precipitation and low-level wind anomaly is unrealistic with enhanced convection occurring within easterly anomalies instead of westerly anomalies as in observations. The over-dependence of precipitation on boundary convergence produced by the MCA scheme is presumably responsible for this unrealistic phase relation in the simulation. The other two schemes produce very poor simulations of the MJO: spectral power of westward propagation is larger than that of eastward propagation in zonal wind and precipitation, indicating a westward propagation of the intraseasonal variability.The mean state and vertical profile of diabatic heating are perhaps responsible for the differences in these simulations. The MCA scheme produces relatively realistic climate background. When either ZM or Tiedtke scheme is used, the observed extension of westerly winds from the western Pacific to the dateline is missing and precipitation over the equatorial region and SPCZ is dramatically underestimated. In addition, diabatic heating produced by both ZM and Tiedtke schemes are very weak and nearly uniform with height. The heating profile produced by the MCA scheme has a middle-heavy structure with much larger magnitude than those produced by the other two schemes. In addition, a very unrealistic boundary layer heating maximum produced by the MCA scheme induces too strong surface convergence, which perhaps contributes to the too strong intraseasonal variability in the simulation. 相似文献
18.
Using the daily average outgoing longwave radiation and NCEP/NCAR reanalysis data in boreal summer (Mays to Octobers) from 1979 to 2007, the propagating characteristics of convection intraseasonal oscillations (ISOs) in the Asian-western Pacific (AWP) region and the relationship between tropical synoptic waves and ISOs are examined by means of finite-domain wavenumber-frequency energy spectrum analysis and lagged linear regression technique. The results are shown as follows. (1) The AWP ISOs propagate both eastward and westward, showing seasonality and regionality. The ISOs propagate eastward with a period of 30 to 60 days over equatorial regions in the whole AWP region, while the westward propagation occurs over 10 to 20? N western Pacific or in the late summers (August, September and October) with periods of 20 to 40 days. The ISOs eastward propagation mainly occurs in primary summers while the westward propagation enhances in late summers. (2) Deep ISO convections associate with westerly and cyclonic circulation anomalies that first form in the Indian Ocean, propagate eastward to the dateline in the Pacific and then turn northwestward. The ISOs convections show northwestward propagating characteristics in the western North Pacific. (3) The ISOs link with the tropical synoptic waves closely. Both convection signals, though with different spatio-temporal scale, enhance simutaneously in the northwestern Pacific, and the ISOs facilitate the forming of a cluster of tropical cyclones (TCs), while a cluster of TCs convection becomes one portion of the northwestward ISOs. 相似文献