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1.
刘一鸣  丁一汇 《气象学报》2001,59(2):129-142
作者在“修正的质量通量积云对流方案及其模拟试验研究I方案介绍及对1991年洪涝过程的模拟”论文中提出的质量通量方案成功地植入区域气候模式RegCM2的基础上,对比分析质量通量方案MFS,Kuo方案和Grell方案对积云对流活动的模拟,结果表明质量通量方案较好地模拟了积云对流活动过程。针对质量通量方案中的一些参数,如云水向雨水的转换率、混合卷入率、混合卷出率和下沉气流的强度等进行了一系列的敏感性试验,试验结果表明积云对流活动对这些参数比较敏感,因此提高这些参数的准确性是改进积云对流参数化方案的重要内容之一。  相似文献   

2.
1991年江淮特大暴雨的降水性质与对流活动   总被引:11,自引:3,他引:11  
从计算大尺度热源和分析TBB资料两个方面,阐述了1991年江淮梅雨期间降水性质与对流活动的季节性演变特征。结果表明:梅雨期间江淮上空3个强上升运动时段分别形成了3场暴雨,由暴雨释放的热量使江淮大气出现了3个时段的强加热;3场暴雨的降水性质呈显著的季节性演变,由第1场暴雨以锋面性降水为主发展到第3场暴雨异常强的对流性降水。文中详细分析了热源和水汽汇的时空分布特征,并从大气运动场和热力结构讨论了盛夏强对流降水期间积云对流以涡动形式对热量和水汽的强铅直输送作用。江淮地区TBB值能很好地反映降水状况,雨期一致地对应于TBB低于250K的时段。梅雨中后期东亚地区对流活动季节性地增强,带状对流区(特别是TBB高负距平区)与雨带位置相符。对流带位置及对流活动强弱与西南暖湿气流活动密切相关,它很好地表征了东亚地区的低空急流(给积云输送热带对流大气)。梅雨期间对流带主要出现在江淮流域,但可在东亚范围内飘移,它落在江淮与否则决定了江淮暴雨的维持与中断  相似文献   

3.
辜旭赞  潘彭刚 《湖北气象》2010,29(2):129-134
采用T213L31模式大气分析资料,诊断计算天气学中的凝结函数降水、水汽通量散度降水,并理想设计与诊断计算气层对流不稳定降水和层结不稳定降水,用于对2007年8月间西太平洋登陆台风帕布和圣帕降水运动进行诊断计算与分析。结果表明:热带扰动中凝结函数降水场呈弱态,但有较强水汽通量散度降水场,且水汽辐合降水运动组织对流不稳定降水和层结不稳定降水。在热带扰动发展与台风形成时,其低层风场水汽辐合与积云对流相互作用的过程,同时是气层对流不稳定能量与气块(团)湿不稳定能量的积聚过程,前者可带来暴雨,后者可带来大暴雨。相关天气学分析表明:台风暴雨是大尺度风场及中尺度水汽辐合降水运动组织起中、小尺度气层、气块(团)对流降水运动,对流性降水是由风场支配故变化较大、较快。  相似文献   

4.
台湾锋前暖区一次积云对流过程   总被引:3,自引:0,他引:3  
冯业荣  罗会邦 《气象学报》1997,55(2):249-250
用TAMEX中尺度试验加密观测资料,研究影响台湾地区的一次梅雨锋前暖区强对流过程,利用积云群整体诊断模式,对积云对流物理过程以及云中参数进行估算,结果给出锋前对流云团与环境场相互作用的物理图像  相似文献   

5.
中尺度数值模式中对流降水参数化方法述评JohnMolinari;MichaelDudek(纽约州立大学大气科学系,奥尔巴尼)1引言在对流不稳定区,质量和湿静力能量的垂直输送不是由天气尺度环流而是由单个积云来完成的。数值模式中积云参数化的概念要求加进这...  相似文献   

6.
本文利用一套具有中尺度分辨率的观测资料,对发生在1983年6月下旬的一次长江流域梅雨暴雨过程进行了诊断研究,并比较了该过程的对流降水活跃期和非活跃期的中尺度环境场特征。结果表明,两个时期的动量场存在明显差异,而水热场差异不大,Q1和Q2以及涡度收支也存在明显差异。在降水活跃期(暴雨集中期),积云对流对能量和涡度的垂直输送有着重要作用;在水热收支中,起主要作用的是垂直输送项,潜热加热基本上为抬升冷却所平衡,水汽的垂直输送是积云对流的主要水汽源;在涡度收支中,低层散度项和扭转项制造正涡度,并通过积云对流向上输送,无论在低层或高层积累的正涡度都被平流非线性过程所耗损。   相似文献   

7.
夏季青藏高原低涡的能量场分析   总被引:3,自引:1,他引:3  
本文采用视热源方程,视水汽汇方程,扰动能量方程和涡度方程对1979年6月的三次低涡进行了分析和研究,得到了以下结论:在低涡生成和发展过程中,积云和乱流引起的总热量的垂直涡旋输送很大。当大气处于条件不稳定时,γs<γ<γα,积云和乱流的这种输送结果,使得低涡的正涡度增长上升到较高层次;另外,积云和乱流对总热量的垂直涡旋输送使得低涡内扰动有效位能增加,然后向扰动动能转换,使低涡得以生成和发展。  相似文献   

8.
积云对流和云物理过程调整对气候模拟的影响   总被引:1,自引:1,他引:0  
本文利用中国科学院大气物理研究所大气科学和地球流体力学数值模拟国家重点实验室 (LASG/IAP) 的大气环流谱模式SAMIL, 结合观测与政府间气候变化专门委员会第四次评估报告 (IPCC AR4) 大气模式集合平均结果, 以大气辐射通量为例, 诊断分析了物理过程调整前后模式对气候模拟的影响。旧版本SAMIL对大气辐射通量的模拟存在较大偏差, 经过大气辐射过程、 积云对流和诊断云等物理过程的调整后, 新版本SAMIL模拟的全球辐射通量的年平均结果与观测的偏差大幅减小, 其中大气顶能量收支的年变化及其平均值与观测更为接近。在积云对流方案调整基础上, 通过对诊断云物理方案的进一步调整, 新版本SAMIL对云物理量模拟更为合理, 在赤道辐合带等区域, 在很大程度上克服了单一积云对流物理过程调整引起的云宏观和微观属性不匹配问题, 能模拟出夏季气候平均辐射通量的全球分布特征, 尤其在东亚区域有较好的模拟能力。研究还表明, 在热带和副热带对流活跃区域, 当前SAMIL中积云对流过程偏差对辐射通量的模拟偏差有很大影响, 而模式中较为简单的诊断云方案也会将云宏观物理量模拟偏差带入云微观量模拟中, 也是主要偏差源之一。本文结果表明, 要继续提高SAMIL的模拟性能, 急需更新云物理参数化方案以改进云辐射过程的模拟, 同时也需要有针对性的研究积云对流和云物理过程之间相互作用, 并作进一步协同调整。  相似文献   

9.
应用常规资料、TBB资料和NCEP分析资料,对2007年7月25日发生在湘黔边境的一次梅雨锋大暴雨天气过程进行了分析.结果表明:深厚的高空低槽和副热带高压稳定维持,有利于冷暖空气的辐合和梅雨锋的长时间维持.梅雨锋上不断有中小尺度对流系统产生,这些中小尺度对流系统在受到大尺度强迫作用和梅雨锋自身的强迫抬升作用而发展增强并长时间维持,在暴雨区形成强烈的降水.暴雨区上空具有低层辐合、高层辐散的结构特征,低层的辐合使得涡度往中上层输送,这种耦合形势有利于垂直上升运动和暴雨的维持.积云对流释放的凝结潜热加热对流层中上层大气,引起梅雨锋锋生,维持和促进了垂直上升运动和对流活动.  相似文献   

10.
本文使用经过青藏高原气象科学实验测站观测资料订正过的欧洲中心FGGE-Ⅲb资料,对1979年夏季青藏高原地区进行了涡度方程诊断分析,研究了它们的月际变化、逐日变化和日变化,与高原上积云对流活动的强弱变化进行了比较,讨论了夏季高原稳定的环流场维持的物理机制;同时还对同时期热带赤道地区强对流活动区域进行了涡度方程诊断分析,将其涡旋环流场的维持机制与夏季高原地区进行了比较. 通过分析,发现夏季青藏高原月平均涡度方程平衡关系主要是次网格尺度项和散度项的平衡,水平平流项的耗散作用在高空较强,但不如次网格尺度项强,涡度方程其余各项均很小.从月际变化、逐日变化和日变化的比较,发现当积云对流活动发生强弱变化时,ω、D和涡度方程中的散度项、次网格尺度项均伴随很强的相应变化,对应关系很好,说明涡度方程中的次网格尺度项R(余差项)的主要部分来源于积云对流系统的活动,反映了夏季高原上存在的强盛频繁的积云对流活动对高原平均环流场的形成和维持具有重要的作用. 使夏季青藏高原高低层环流场加强的物理机制足高低层气流强大的辐散辐合,耗散机制是积云对流系统对高低层涡度的上下搅拌垂直输送作用和网格尺度水平平流项的非线性耗散作用,其中前者起主要的作用. 从涡旋能量维持的角度看,夏季青藏高原高低层环流场的维持大致是高原尺度环流系统的涡旋能量通过非线性过程,分别向高原区域以外更大尺度的系统和次网格尺度的对流系统输送,输送的损失由强大的高低层辐散辐合气流产生的涡旋能量补充,从而维持了高原地区环流场的稳定.赤道附近热带强对流活动区域环流场的维持机制与夏季高原地区的不同点,主要表现在其高层和低层的区域尺度环流场通过非线性作用都从更大尺度环流场得到涡旋能量,并把涡旋能量转送给次网格尺度积云对流系统,使自身维持稳定.  相似文献   

11.
The diagnostic model of the cumulus convection proposed by Yanai et al. (1973) was applied to the atmosphere over the Tibetan Plateau, and used to estimate the vertical mass flux, entrainment and detrainment, excess temperature and moisture, liquid water content, and condensation and precipitation rates of highland cloud clusters. The re-sults illustrated that in clouds over the Tibetan Plateau, the water vapor condensation rate, liquid water content, and efficiency of the rain generation process are less than those in the tropics (represented by the Marshall Islands region). Therefore, the condensational latent heat released over the Tibetan Plateau, overall, is much smaller than that in the tropics. The water vapor and liquid water detrainment from shallow nonprecipitating cumulus clouds, and their entrainment into deep cumulus clouds, serve as a growing mechanism for the deep precipitating cumulus towers over the Tibetan Plateau. It should be noted that there is a stronger detrainment of liquid water from cumulus clouds and a stronger re-evaporation rate in environment. The process of the condensation-detrainment-re-evaporation-entrainment is repeatedly in progress. It would play an important role in maintaining of cumulus convection on the condition that the supply of moisture is not plentiful over the Tibetan Plateau.The analyses also showed that the cloud mass flux Mc over the Tibetan Plateau is less, and the large-scale av-erage upward motion is much less than those over the Marshall Islands. Stronger compensating downward motion in the cloud environment over the Tibetan Plateau, responsible for the area’s strong environmental heating rate was re-vealed, and would link to the stability of the South Asian High in summer.  相似文献   

12.
梅雨锋云带内α-中尺度对流系统周边水汽风的分析   总被引:4,自引:0,他引:4  
刘启汉  陈受钧 《气象学报》2004,62(2):237-242
应用准静止卫星水汽图像导出的风 (简称为水汽风 )分析东亚梅雨锋云带内中尺度对流系统 (MCS)在对流层上层的流出通道。结果表明梅雨锋云带内MCS有二类流出通道。一类MCS在对流层上层呈现为一个中尺度反气旋。MCS的东部有一支中尺度高空急流 ,这支中尺度高空急流向东流出后转向南 ,流入 2 0°N附近的南亚东风急流内 ,是MCS在对流层上层的主要流出通道。另一类MCS发生在中纬度西风急流的南侧。中纬度西风与MCS南部的偏东北风构成一个反气旋环流带。MCS前方的流出通道 (中尺度高空急流 )是中纬度西风急流的一个中尺度分支。梅雨锋云带内垂直方向水平风速切变小于 1m/ (s·10 0hPa) ,垂直方向“不通风”有利于云带内MCS的维持。初步分析验证了以前数值模拟得到的中尺度高空急流及其流出通道。  相似文献   

13.
Impact of increased vertical resolution on simulation of tropical climate   总被引:1,自引:0,他引:1  
Summary The aim of this study is to describe the behaviour of tropical dynamics in the ECHAM4 model when increased vertical resolution around the tropopause and in the planetary boundary layer is used. In this work we perform experiments with the ECHAM4 model using T30 horizontal resolution and 19 and 42 vertical levels. The impact of the increased vertical resolution on the simulation of tropical clouds and precipitation has been investigated. Therefore, the dynamic fields related to tropical convection have been analyzed. The results suggest a beneficial effect of the increased number of vertical levels on the convective scheme performance and on the related dynamic fields over the Tropics. The improvement of the rainfall climatologies in the 42-level model has been explained via the impact of vertical resolution on the cloud structure. In the cloud spectrum of the L42 simulation, a third peak appears around 600 hPa, revealing that when using higher vertical resolution the convective parametrization starts to represent cumulus congestus clouds.  相似文献   

14.
This paper aims at characterizing how different key cloud properties (cloud fraction, cloud vertical distribution, cloud reflectance, a surrogate of the cloud optical depth) vary as a function of the others over the tropical oceans. The correlations between the different cloud properties are built from 2?years of collocated A-train observations (CALIPSO-GOCCP and MODIS) at a scale close to cloud processes; it results in a characterization of the physical processes in tropical clouds, that can be used to better understand cloud behaviors, and constitute a powerful tool to develop and evaluate cloud parameterizations in climate models. First, we examine a case study of shallow cumulus cloud observed simultaneously by the two sensors (CALIPSO, MODIS), and develop a methodology that allows to build global scale statistics by keeping the separation between clear and cloudy areas at the pixel level (250, 330?m). Then we build statistical instantaneous relationships between the cloud cover, the cloud vertical distribution and the cloud reflectance. The vertical cloud distribution indicates that the optically thin clouds (optical thickness <1.5) dominate the boundary layer over the trade wind regions. Optically thick clouds (optical thickness >3.4) are composed of high and mid-level clouds associated with deep convection along the ITCZ and SPCZ and over the warm pool, and by stratocumulus low level clouds located along the East coast of tropical oceans. The cloud properties are analyzed as a function of the large scale circulation regime. Optically thick high clouds are dominant in convective regions (CF?>?80?%), while low level clouds with low optical thickness (<3.5) are present in regimes of subsidence but in convective regimes as well, associated principally to low cloud fractions (CF?<?50?%). A focus on low-level clouds allows us to quantify how the cloud optical depth increases with cloud top altitude and with cloud fraction.  相似文献   

15.
Based on the two-dimensional slab-symmetric model of cumulus clouds established by the authors,thedevelopment of the cumulus cloud and its precipitation in environments with and without the stratiform cloudpresent has been simulated numerically in almost the same atmospheric stratification.Results show that thepresence of the stratiform cloud has a significant effect on the development of the cumulus cloud and theincreae of its precipitation.The rainfall may increase by scveral to tens of times.It is believed that theconvective-stratiform mixed cloud system may be important for producing heavy to torrential rain.This isin good agreement with what has been observed in the Meiyu frontal cloud system in recent investigations  相似文献   

16.
 Experiments using a GCM with two different vertical resolutions show differences in the amount of variability in the tropical upper tropospheric zonal wind component associated with the Madden-Julian Oscillation (MJO). The GCM with lower vertical resolution shows very little variability in this quantity whereas when the vertical resolution is doubled in the free troposphere, the GCM produces variability which is of the same strength as observations. However, the eastward propagation of an enhanced convective region from the Indian Ocean into the west Pacific is not well represented in either simulation of this atmospheric GCM. A water-covered or “aqua-planet” version of the same GCM is used to investigate the behaviour of tropical convection when the vertical resolution is doubled. When the vertical resolution is increased, the spectrum of tropical cloud types changes from a bimodal distribution with peaks representing shallow cumulus and deep cumulonimbus clouds to a trimodal distribution with a third peak in mid-troposphere near the melting level. Associated with periods when these mid-level congestus clouds are dominant, the detrainment from these clouds significantly moistens the mid-troposphere. The appearance of these congestus clouds is shown to be partly due to improved resolution of the freezing level and the convective processes occurring at this level. However, due to the way in which convective detrainment is parametrized in this model, the vertical profile becomes rather noisy and this too contributes to the change in the nature of the convective clouds. The resulting cloud distribution more closely resembles observations, particularly during the suppressed phase of the MJO when cumulus congestus is the dominant cloud type. Received: 17 April 2000 / Accepted: 30 November 2000  相似文献   

17.
不同降水方案对"03.7"一次暴雨过程模拟的影响   总被引:4,自引:0,他引:4  
观测和数值模拟研究已经表明,潜热释放对中国东部夏季梅雨锋系统及其锋面降水的维持和发展发挥着非常重要的作用.然而,目前对于梅雨锋降水模拟中各种降水方案的相互协调和系统评估方面的工作仍不多见,为了增进对梅雨锋暴雨模拟中降水过程的认识,作者针对2003年7月4~5日一次梅雨锋暴雨过程,构造了四组试验,利用MM5模式考察了两种分辨率(36 km、12 km),各种隐/显式方案搭配下,对所生成的雨带、雨量和降水类型的配置进行了仔细的研究,得到了一些有意义的结论,为今后更好地使用模式、利用数值模式来认识中尺度降水过程中的气象问题打下基础.主要结论包括:模拟总降水的水平分布和强度,以及显式降水和隐式降水的划分对积云参数化方案的选择非常敏感.但对特定积云参数化方案而言,降水的模拟对36 km、12 km水平分辨率不敏感(除Betts-Miller方案外);在中尺度网格分辨率10~50 km范围内,不同积云参数化方案对梅雨锋降水分布和降水量模拟的影响比不同显式方案带来的变化大得多.  相似文献   

18.
Mesoscale cellular convections over the East China Sea during cold air outbreaks are simulated with a high-resolution numerical model. The model incorporates important physical processes involved in shallow convection, such as the exchange of heat and moisture between water and air; condensation; evaporation; and vertical turbulent transfer of heat, moisture, and momentum.The results show that open cells develop with aspect ratios as large as 14. The structure of the convection is examined in detail. The organized mesoscale circulation is responsible for breaking up the initial stratus cloud deck and enhancing turbulence in the upward-moving area (especially inside cumulus clouds). However, it is found that the heat flux contributed by MCC's themselves is much smaller than the eddy heat flux.  相似文献   

19.
For numerical weather prediction models and models resolving deep convection, shallow convective ascents are subgrid processes that are not parameterized by classical local turbulent schemes. The mass flux formulation of convective mixing is now largely accepted as an efficient approach for parameterizing the contribution of larger plumes in convective dry and cloudy boundary layers. We propose a new formulation of the EDMF scheme (for Eddy Diffusivity\Mass Flux) based on a single updraft that improves the representation of dry thermals and shallow convective clouds and conserves a correct representation of stratocumulus in mesoscale models. The definition of entrainment and detrainment in the dry part of the updraft is original, and is specified as proportional to the ratio of buoyancy to vertical velocity. In the cloudy part of the updraft, the classical buoyancy sorting approach is chosen. The main closure of the scheme is based on the mass flux near the surface, which is proportional to the sub-cloud layer convective velocity scale w *. The link with the prognostic grid-scale cloud content and cloud cover and the projection on the non- conservative variables is processed by the cloud scheme. The validation of this new formulation using large-eddy simulations focused on showing the robustness of the scheme to represent three different boundary layer regimes. For dry convective cases, this parameterization enables a correct representation of the countergradient zone where the mass flux part represents the top entrainment (IHOP case). It can also handle the diurnal cycle of boundary-layer cumulus clouds (EUROCS\ARM) and conserve a realistic evolution of stratocumulus (EUROCS\FIRE).  相似文献   

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