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1.
青藏高原一次强对流过程对水汽垂直输送的数值模拟   总被引:1,自引:0,他引:1  
朱士超  银燕  金莲姬 《大气科学》2011,35(6):1057-1068
本文采用中尺度天气研究预测模式(WRF)模拟了青藏高原那曲地区的一次强对流过程,分析了强对流对水汽的垂直输送量及对模式不同云微物理参数化方案的敏感性.通过与实测资料的比较,发现此次模拟在对流发生时间、地点、降水时间等方面均与实际接近.敏感性试验表明:当对流发生时,对流区域向上的水汽通量随海拔高度呈先增大后减小的趋势,该...  相似文献   

2.
两种短期降水集合预报方案的对比试验   总被引:2,自引:1,他引:1  
将MM5V3作为试验模式,利用初值扰动和物理参数化方案,分别对东南沿海地区2004年7—9月的短期降水进行了模拟,并运用均方根误差法对模拟试验效果进行了评估检验,以比较两种方案的集合预报效果。结果表明,对于汛期短期降水预报而言,两种方案的预报效果都有一定的改进。相对于初值误差而言,积云对流过程在汛期降水过程中起着更为重要的作用,因而物理参数化方案扰动的集合预报效果,总体优于基于初值扰动的集合预报效果。研究还发现,模式物理参数化方案扰动的集合预报效果在9月出现了明显的下滑,这主要由于7—8月对流活动旺盛,而9月对流活动随热力因素减弱而减弱的原因所致。  相似文献   

3.
Uncertainties in simulating the seasonal mean atmospheric water cycle in Equatorial East Africa are quantified using 58 one-year-long experiments performed with the Weather Research and Forecasting model (WRF). Tested parameters include physical parameterizations of atmospheric convection, cloud microphysics, planetary boundary layer, land-surface model and radiation schemes, as well as land-use categories (USGS vs. MODIS), lateral forcings (ERA-Interim and ERA40 reanalyses), and domain geometry (size and vertical resolution). Results show that (1) uncertainties, defined as the differences between the experiments, are larger than the biases; (2) the parameters exerting the largest influence on simulated rainfall are, in order of decreasing importance, the shortwave radiation scheme, the land-surface model, the domain size, followed by convective schemes and land-use categories; (3) cloud microphysics, lateral forcing reanalysis, the number of vertical levels and planetary boundary layer schemes appear to be of lesser importance at the seasonal scale. Though persisting biases (consisting of conditions that are too wet over the Indian Ocean and the Congo Basin and too dry over eastern Kenya) prevail in most experiments, several configurations simulate the regional climate with reasonable accuracy.  相似文献   

4.
The application of the single Doppler radar dataset analysis is usually confined to the assumption that the actual wind is linearly distributed or uniform locally.Following some dynamic features of convective weather,a conceptual model of moderate complexity is constructed,wherewith a horizontal wind perturbation field is retrieved directly from the single Doppler radar measurements.The numerical experiments are based on a 3-D cloud model-generated convective cell,whose radial velocity component is taken as the radar observations that are put into the closed equations based on the conceptual model to retrieve the horizontal wind perturbation field.After the initial field is properly treated,the retrieval equation is solved in terms of the 2-D FFT technique and the sensitivity to noise is examined.Finally,contrast analysis is done of the retrieved and the cloud model output wind fields,indicating the usefulness of the approach proposed in this paper.  相似文献   

5.
The application of the single Doppler radar dataset analysis is usually confined to the assumption that the actualwind is linearly distributed or uniform locally.Following some dynamic features of convective weather,a conceptualmodel of moderate complexity is constructed,wherewith a horizontal wind perturbation field is retrieved directly fromthe single Doppler radar measurements.The numerical experiments are based on a 3-D cloud model-generatedconvective cell,whose radial velocity component is taken as the radar observations that are put into the closed equationsbased on the conceptual model to retrieve the horizontal wind perturbation field.After the initial field is properlytreated,the retrieval equation is solved in terms of the 2-D FFT technique and the sensitivity to noise is examined.Finally,contrast analysis is done of the retrieved and the cloud model output wind fields,indicating the usefulness of theapproach proposed in this paper.  相似文献   

6.
对流尺度数值预报中的云物理初始化方法改进及个例试验   总被引:2,自引:0,他引:2  
李佳  陈葆德  黄伟  张旭 《气象学报》2017,75(5):771-783
通过在云初始化方案中增加由地表感热和潜热通量确定的对流尺度速度作为对流判据,同时增加层云云冰、云水计算方案,改进云分析方法,并基于第2代华东快速更新循环同化模式预报系统,针对2015年4月28日华东强对流个例,进行对比试验,分析了改进的云初始化方案对云分析结果和模式预报效果的影响。试验表明:在云分析中增加对流判据,使得平均40%左右的云分析格点判定为非对流格点,对流格点分布与正的感热通量分布相似,在陆地上有显著日变化。在对流和层云格点判定之后,增加层云云冰、云水计算方案分析层云格点,显著地减小了模式初始场的云冰、云水混合比,有效地减弱了模式积分初始阶段云冰、云水含量的剧烈调整,尤其是在陆地区域。采用改进的云初始化方案进行预报,可以减少模式前1 h和前6 h的降水强度;尤其在个例的循环试验中,强降水中心强度和面积的预报比原方案显著减弱。   相似文献   

7.
高纬度强对流与对流层上层水汽变化关系的数值模拟研究   总被引:2,自引:2,他引:0  
应用WRF中尺度模式模拟了发生在黑龙江省西南部的一次区域性暴雨过程,通过云微物理参数化方案的敏感性试验,分析了对流云体中水汽垂直输送特征.结果表明:强对流活动使对流层上层局地水汽平均增加10倍以上,对流活动对于水汽的垂直输送以及对高层水汽含量的改变具有非常显著的作用.云微物理参数化方案,对于整个对流层水汽通量密度变化趋势有较好的表现.在不同方案中,0.5 ~9 km水汽通量密度及24 h总水汽垂直输送量,随高度变化差异较大.这是由平均垂直速度对不同方案敏感性造成的,不同的参数化方案,水汽通量最大值间最多相差可达27.9%.在不同的方案中,对流层上层加湿作用持续时间和对流层上层平均水汽混合比的最大值较敏感:对流活动可造成模拟区域对流层上层增湿持续16 ~20 h不等;对流层上层平均水汽混合比的最大值差异明显,最大可达15.8%.进行24 h平均后,上述物理量对方案的敏感性可减小到8.3%.所以,云微物理方案的不确定性对于暴雨过程的时间尺度是不可忽视的.  相似文献   

8.
Numerical simulation of meso-β-scale convective cloud systems associated with a PRE-STORM MCC case has been carried out using a 2-D version of the CSU Regional Atmospheric Modeling System (RAMS) nonhydrostatic model with parameterized microphysics. It is found that the predicted meso-γ-scale convective phenomena are basically unsteady under the situation of strong shear at low-levels, white the meso-β-scale convective system is maintained up to 3 hours or more. The meso-β-scale cloud system exhibits characteristics of a multi-celled convective storm in which the meso-γ-scale convective cells have lifetime of about 30 min. Pressure perturbation depicts a meso-low after a half hour in the low levels. As the cloud system evolves, the meso-low inten-sifies and extends to the upshear side and covers the entire domain in the mid-lower levels with the peak values of 5-8 hPa. Temperature perturbation depicts a warm region in the middle levels through the entire simulation period. The meso-γ-scale warm cores with peak values of 4-8oC are associated with strong convective cells. The cloud top evapo-ration causes a stronger cold layer around the cloud top levels.Simulation of microphysics exhibits that graupel is primarily concentrated in the strong convective cells forming the main source of convective rainfall after one hour of simulation time. Aggregates are mainly located in the stratiform region and decaying convective cells which produce the stratiform rainfall. Riming of the ice crystals is the predominant precipitation formation mechanism in the convection region, whereas aggregation of ice crystals is the predominant one in the stratiform region, which is consistent with observations. Sensitivity experiments of ice-phase microphysical processes show that the microphysical structures of the convective cloud system can be simulated better with the diagnosed aggregation collection efficiencies.  相似文献   

9.
 A method is described for evaluating the ‘partial derivatives’ of globally averaged top-of-atmosphere (TOA) radiation changes with respect to basic climate model physical parameters. This method is used to analyse feedbacks in the Australian Bureau of Meteorology Research Centre general circulation model. The parameters considered are surface temperature, water vapour, lapse rate and cloud cover. The climate forcing which produces the changes is a globally uniform sea surface temperature (SST) perturbation. The first and second order differentials of model parameters with respect to the forcing (i.e. SST changes) are estimated from quadratic least square fitting. Except for total cloud cover, variables are found to be strong functions of global SST. Strongly non-linear variations of lapse rate and high cloud amount and height appear to relate to the non-linear response in penetrative convection. Globally averaged TOA radiation differentials with respect to model parameters are also evaluated. With the exception of total cloud contributions, a high correlation is generally found to exist, on the global mean level, between TOA radiation and the respective parameter perturbations. The largest non-linear terms contributing to radiative changes are those due to lapse rate and high cloud. The contributions of linear and non-linear terms to the overall radiative response from a 4 K SST perturbation are assessed. Significant non-linear responses are found to be associated with lapse rate, water vapour and cloud changes. Although the exact magnitude of these responses is likely to be a function of the particular model as well as the imposed SST perturbation pattern, the present experiments flag these as processes which cannot properly be understood from linear theory in the evaluation of climate change sensitivity. Received: 16 January 1997/Accepted: 9 May 1997  相似文献   

10.
In the context of non-hydrostatic MM5 version we have explored the impact of convective parameterization schemes on uncertainty in mesoscale numerical prediction of South China heavy rain and mesoscale heavy rainfall short-range ensemble simulation by using two kinds of physics perturbation methods through a heavy rain case occurring on June 8, 1998 in Guangdong and Fujian Provinces. The results show the physical process of impacts of convective schemes on heavy rainfall is that different latent heat of convective condensation produced by different convective schemes can make local temperature perturbation, leading to the difference of local vertical speed by the intrinsic dynamic and thermodynamic processes of atmosphere,and therefore, making difference of the timing, locations and strength of mesh scale and subgrid scale precipitation later. New precipitations become the new source of latent heat and temperature perturbation,which finally make the dynamic and thermodynamic structures different in the simulations. Two kinds of methods are used to construct different model version stochastically. The first one is using different convective parameterization and planetary boundary layer schemes, the second is adjusting different parameters of convective trigger functions in Grell scheme. The results indicate that the first ensemble simulations can provide more uncertainty information of location and strength of heavy rainfall than the second. The single determinate predictions of heavy rain are unstable; physics ensemble predictions can reflect the uncertainty of heavy rain, provide more useful guidance and have higher application value.Physics ensembles suggest that model errors should be taken into consideration in the heavy rainfall ensembles. Although the method of using different parameters in Grell scheme could not produce good results, how to construct the perturbation model or adjust the parameter in one scheme according to the physical meaning of the parameter still needs further investigation. The limitation of the current study is that it is based on a single case and more cases will be addressed in the future researches.  相似文献   

11.
我国西部高原大气边界层中的对流活动   总被引:4,自引:0,他引:4       下载免费PDF全文
利用 1 998年第 2次青藏高原野外试验中的多普勒声雷达探测、低空探测观测以及卫星观测资料对高原大气边界层内的对流现象进行分析研究。声雷达探测到了高原边界层内有强烈的对流活动。这种对流泡中心的垂直速度可超过 1m/s,并存在尺度为 1个多小时的周期性 ,表现为中小尺度的有组织的湍流活动。高原边界层强对流得以发展和维持的物理机制是 :强辐射加热、复杂的地形地貌形成的下垫面不均一性造成边界层斜压性、边界层内的平流活动等 ,这些现象都有利于对流的发展。在这些条件的作用下 ,边界层内可以产生一系列有组织的强湍流大涡旋活动 ,这些大涡旋形成的热泡在向上发展的过程中有的能够发生合并 ,变得更大也更为猛烈 ,达到凝结高度以上可形成对流云 ,并发生充分的对流混合。成云过程凝结潜热释放更有利于对流运动进一步发展 ,使对流云逐步发展成更大的对流云团 ,从而产生卫星云图中显示的云团发展过程。  相似文献   

12.
A heavy rainfall in the Meiyu front during 4--5 July 2003 is simulated by use of the non-hydrostatic mesoscale model MM5 (V3--6) with different explicit cloud microphysical parameterization schemes. The characteristics of microphysical process of convective cloud are studied by the model outputs. The simulation study reveals that: (1) The mesoscale model MM5 with explicit cloud microphysical process is capable of simulating the instant heavy rainfall in the Meiyu front, the rainfall simulation could be improved significantly as the model resolution is increased, and the Goddard scheme is better than the Reisner or Schultz scheme. (2) The convective cloud in the Meiyu front has a comprehensive structure composed of solid, liquid and vapor phases of water, the mass density of water vapor is the largest one in the cloud; the next one is graupel, while those of ice, snow, rain water and the cloud water are almost same. The height at which mass density peaks for different hydrometeors is almost unchangeable during the heavy rainfall period. The mass density variation of rain water, ice, and graupel are consistent with that of ground precipitation, while that of water vapor in the low levels is 1--2 h earlier than the precipitation. (3) The main contribution to the water vapor budget in the atmosphere is the convergence of vapor flux through advection and convection, which provides the main vapor source of the rainfall. Besides the basic process of the auto-conversion of cloud water to rain water, there is an additional cloud microphysical process that is essential to the formation of instant heavy rainfall, the ice-phase crystals are transformed into graupels first and then the increased graupels mix with cloud water and accelerates the conversion of cloud water to rain water. The positive feedback mechanism between latent heat release and convection is the main cause to maintain and develop the heavy precipitation.  相似文献   

13.
一次MCS过程的卫星云图和数值模拟分析   总被引:1,自引:4,他引:1       下载免费PDF全文
本文应用卫星云图与数值模拟结果对2000年6月2日发生的一次影响江苏的江淮气旋暴雨过程进行研究分析,阐述了这次暴雨过程表现的MCS基本特征。分析表明:MCS的形成可以由几个中β尺度对流云或对流带开始,在特定的环境场中汇合成合并;在其发展过程中必须维持湿度平流,低层到中层有暖平流,骨强偏南风急流伸向形成区,同时在其东北方向有一支高空西风急流相耦合;低层的辐合、整层凝结潜热的释放、垂直运动的增强、高层的辐散引起的正反馈机制是MCS发展的动因。  相似文献   

14.
本文对GRAPES_Meso中Kain-Fritcsh eta积云参数化方案进行了三种改进:(1)将原触发机制中的温度扰动分解成由水汽决定的垂直向和水平向温度扰动(KF1方案),(2)在原温度扰动中直接增加一项由相对湿度计算的水汽平流项(KF2方案),(3)在KF1方案中增加用相对湿度计算的水汽平流项(KF3方案)。利用GFS预报场资料对上述改进方案进行模拟试验和批量回报试验,结果表明:“5·23”暴雨个例中,(1)改进方案均可以减少原方案模拟的部分虚假降水,KF1方案模拟降水范围较好,KF2方案模拟强降水中心较好,KF3方案同时具备二者优点。(2)三种改进方案对于强降水站点均存在模拟降水偏弱,KF1方案降水趋势与实况接近,但存在对流激发较快,后期降水略为不足,KF2方案则相反,KF3方案表现介于二者之间;KF2、KF3方案均会在对流激发最强和最弱时刻使其向有利方向调整。台风个例中,KF1方案模拟中心气压较好,KF2方案模拟台风路径较好,KF3方案则在两者上均有较好表现。TS评分检验表明KF1方案在各个降水量级上的评分都较低,KF2、KF3方案评分相对较高;误差检验(高度、风)时,KF1方案在中层误差较大,高、低层误差最小,其他两种方案表现则相反。   相似文献   

15.
华南中尺度暴雨数值预报的不确定性与集合预报试验   总被引:50,自引:0,他引:50  
陈静  薛纪善  颜宏 《气象学报》2003,61(4):432-446
利用非静力MM5模式,分析了不同积云对流参数化方案对华南暖区暴雨数值预报的不确定性影响,进行了中尺度暴雨模式扰动集合预报试验。不同对流参数化方案的对流凝结加热引起不同的局地温度扰动,通过大气内部的热力动力过程,导致垂直速度的差异,进而影响网格尺度和次网格尺度降水时间、地点和强度。后续降水再通过凝结潜热释放形成新的扰动源。不同积云对流参数化方案还可引起扰动源能量传播方式不同,最终使模拟大气的动力和热力结构有差异。针对物理过程的不确定性,使用两种模式扰动方法构造集合预报扰动模式,第一种方法是随机组合不同积云对流参数化方案和边界层方案,第二种方法是扰动Grell积云对流参数化方案中主要参数振幅。集合预报结果表明,第一种方法的集合预报效果优于第二种方法,仅扰动参数振幅值似乎还不足以反映华南暴雨预报的不确定性。单一的确定性预报在暴雨落区和强度方面的可信度不稳定,集合产品能给华南暴雨过程提供更有用价值的指导预报,具有较高的应用价值。  相似文献   

16.
积层混合云结构特征及降水机理的个例模拟研究   总被引:2,自引:1,他引:1  
何晖  高茜  刘香娥  周嵬  贾星灿 《大气科学》2015,39(2):315-328
积层混合云是我国一种重要的降水系统, 其降水既有对流云又有层状云特征。基于积层混合云的重要性, 本文利用中尺度数值模式WRF(Weather Research and Forecasting Model), 结合三维粒子运行增长模式对2012年5月29日北京地区的一次积层混合云降过程进行了模拟研究。模拟的降水与雷达回波与实测结果基本一致。在此基础上, 重点分析了混合云系中积状云与层状云各自的微物理结构特征与降水的发生机理等。结果表明:降水过程云内存在着明显的“播种—供给”机制, 层状云中“播种—供给”机制相对简单。而对流云区中由于降水粒子可以发生上下多次的循环增长, “播种—供给”机制可在云的上下层间双向进行, 云中粒子群可以增长得更大。在积层混合云中, 在低层, 层状云中已有的水凝物粒子进入内嵌的积云块中, 而在高层水成物粒子又从积云中落到层云中, 积层混合云系充分发挥了积云和层云各自的优势, 从而降水效率较高。  相似文献   

17.
云微物理参数化对华北降雪影响的数值模拟   总被引:7,自引:3,他引:7  
对发生在华北地区的一次降雪过程进行了中尺度数值模拟。结果表明,高纬强冷空气南下和低纬倒槽的水汽输送是造成这次长时间降雪过程的主要原因。采用混合方案的中尺度数值模拟表明,这次降雪天气不是对流云造成的,而是稳定性的非对流云降雪。敏感性试验也表明,采用其他积云参数化方案对模拟的降雪量基本没有影响。控制试验模拟的24h降雪量与实际观测比较吻合。模拟结果表明,当采用Dudhia简单冰相方案时,会有过多的云冰、过冷却水及雪;当采用Reisner 1混合相方案时,会有过多的云冰和雪;修改的各个Reisner 2方案对此次降雪的预报改进不大,但各个Reisner 2方案的敏感性试验中云冰混合比、过冷却水混合比和雪混合比稍微有差异。  相似文献   

18.
本文利用WRF(Weather Research and Forecasting)模式的不同云微物理方案对2009年6月14日发生在华东地区的一次飑线过程进行1 km的高分辨率模拟,探讨不同云微物理方案对飑线模拟的影响。结果表明:双参数方案的模拟效果总体上优于单参数方案,其中WDM6方案模拟效果最佳,能够较好的模拟出强对流回波区、层云区的主要特征。在单参数方案中以WSM6方案最优。Kessler和LIN方案模拟飑线的回波范围偏小,强度偏弱。进一步对比热力和动力场发现,WDM6方案模拟的冷池的面积最大,强度最强,气压最高,飑线前部的入流处风速最大。不同云微物理方案对微物理场的影响较明显,相比单参数方案,双参数方案模拟的水凝物混合比更高,且能够模拟粒子数浓度,更准确地描述了云中的各类粒子特征。  相似文献   

19.
一次梅雨锋暴雨云物理特征的数值模拟研究   总被引:4,自引:1,他引:3  
鞠永茂  王汉杰  钟中  宋帅 《气象学报》2008,66(3):381-395
利用中尺度数值模式MM5(V3.6),选用模式中不同的显式云物理方案,对2003年7月4-5日发生在江淮流域的梅雨锋暴雨过程进行了数值模拟,并根据模拟结果对造成此次暴雨过程的对流云团的微物理特征进行了分析.研究结果表明:(1) 具有详细云物理过程的中尺度模式MM5对短时强降水过程具有较好的模拟能力,提高MM5模式的分辨率,可以更好地模拟短时梅雨锋暴雨过程,模式中的Goddard云物理方案的模拟结果要优于Reisner方案和Schultz方案.(2) 梅雨锋对流云团是一种复杂的固、液、气三相混合体结构,在云体区域内的平均质量密度分布中,水汽的质量密度最大,其次是霰,而冰晶、雪、云水和雨水的质量密度较小且数值大小彼此接近,各种相态粒子质量密度峰值出现的高度随时间无明显变化.雨水、云冰和霰的质量密度随时间演变规律与地面降水强度的变化特征相一致,近地面层水汽密度随时间的演变规律比地面降水强度提前1-2个小时,水汽通量的辐合对暴雨时段内水汽的补充和维持起到了重要的作用.(3) 除了最基本的云水向雨水转化的云微物理过程之外,此次降水过程还显示,在中层500-700 hPa范围内雪、冰晶等冰相粒子首先转化为霰粒子,而霰和云水的结合进一步加速(剧)云水向雨水的转换,成为短时特大暴雨形成不可或缺的动力机制,云物理过程中的相变潜热与对流运动的正反馈机制是促进暴雨维持和发展的最重要热力因子.  相似文献   

20.
使用中尺度数值模式WRF中的双参数云微物理方案WDM6针对2008年台风“凤凰”登陆过程中造成的强降水进行数值模拟,通过卫星模拟器利用MTSAT-1R和TRMM卫星观测的红外云顶黑体亮温TBB、PR雷达反射率资料使用统计方法验证模拟结果。通过修改云水向雨水自动转化过程、冰晶核化过程、雪和霰的下落末速度、雪和霰的截距进行敏感性试验,减小模拟结果和卫星观测结果的差异。研究结果表明:WDM6方案模拟的台风“凤凰”登陆后的降水,强对流云系及对流柱状雷达回波基本符合实况,但模拟结果局部偏强。WDM6方案模拟产生了较多的浅对流云,低估了对流云系的出现频率。不同云类型模拟的雷达回波均偏强,对流云系雷达回波垂直分布接近观测。敏感性试验结果说明修改WDM6方案中云水向雨水自动转化率有效地改善了模拟效果。同时发现云滴初始数浓度影响云水向雨水自动转化率并最终影响云系结构和雷达反射率的模拟结果,过高的云滴初始数浓度会使模拟结果变差。  相似文献   

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