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A 3-year Mesoscale Convective Systems (MCSs) database, which extends from 2000 to 2002, has been built for the Iberian Peninsula and the Balearic Islands using the objective method MASCOTTE (MAximum Spatial COrrelation Technique). It was originally developed to track the evolution of convective systems over the Amazon region; after modifications, it is able to track MCS evolution even with an hour and a half of missed images and provides essential information of both dynamical and morphological characteristics of MCSs. MASCOTTE is tested against a visual and subjective method, and is found to offer advantages such as automation and a simple and efficient operation that make it very useful for building large MCS databases.Thirty-five MCSs were found between June and October, most of them originated along the Mediterranean coast and near the Pyrenees, showing an increasing occurrence from June to September, when the maximum is found. The regions most influenced by MCS occurrences are Balearic Islands, Valencia, Catalonia, Murcia and the Basque Country. The MCSs tend to be small, short-lived and linear, usually moving eastward or northeastward with low velocities.The MCSs-associated precipitation presents high variability, ranging from 80 to 0 mm h−1 as maximum hourly records. Two different convective regions are identified based on MCS behavior in extreme precipitation events: Northern Spain (the Basque Country) with abundant and continuous precipitation regime but little MCS influence, and the Mediterranean coast, where precipitation is sporadic but much more intense.  相似文献   
23.
A parallelized large-eddy simulation model has been used to investigate the effects of two-dimensional, discontinuous, small-scale surface heterogeneities on the turbulence structure of the convective boundary layer.Heterogeneities had a typical size of about the boundary-layer heightzi. They were produced by a surface sensible heat flux pattern ofchessboard-type and of strong amplitude as typical, e.g., for the marginalice zone. The major objectives of this study were to determinethe effects of such strong amplitude heat flux variations and to specify theinfluence of different speeds and directions of the background wind.Special emphasis has been given to investigate the secondary circulations induced by the heterogeneities by means of three-dimensional phase averages.Compared with earlier studies of continuous inhomogeneities, the same sizeddiscontinuous inhomogeneities in this study show similar but stronger effects.Significant changes compared with uniform surface heating are only observedwhen the scale of the inhomogeneities is increased to zi. Especially the vertical energy transport is much more vigorous and even the mean emperature profile shows a positive lapse rate within the whole mixed layer. However, the effects are not directly caused by the different shape of the inhomogeneities but can mainly be attributed to the large amplitude of the imposed heat flux,as it is typical for the partially ice covered sea during cold air outbreaks.The structure of the secondary flow is found to be very sensitive to the wavelength and shape of the inhomogeneities as well as to the heatflux amplitude, wind speed and wind direction. The main controlling parameter is the near-surface temperature distribution and the related horizontal pressure gradient perpendicular to the main flow direction. The secondary flow varies from a direct circulation with updraughts mainly above the centre of the heated regions to a more indirect circulation with updraughts beneath the centre and downdraughts above it. For background winds larger than 2.5 m s–1 a roll-like circulation pattern is observed.From previous findings it has often been stated that moderate backgroundwinds of 5 m s–1 eliminate all impacts of surface inhomogeneitiesthat could potentially be produced in realistic landscapes. However, this studyshows that the effects caused by increasing the wind speed stronglydepend on the wind direction relative to the orientation of theinhomogeneities. Secondary circulations remain strong, even for abackground wind of 7.5 m s–1, when the wind direction is orientatedalong one of the two diagonals of the chessboard pattern. On the otherhand, the effects of inhomogeneities are considerably reduced, even undera modest background wind of 2.5 m s–1, if the wind direction isturned by 45°. Mechanisms for the different flow regimesare discussed.  相似文献   
24.
对流性强风暴系统的螺旋度动力学研究   总被引:14,自引:0,他引:14  
利用风暴尺度的数值模式ARPS成功地模拟了1977年5月20日在美国Oklahoma州Del City的一次强对流风暴过程。其模拟结果与实际的观测非常接近,模式积分 40分钟,初始对流单体发生了分裂,产生了新的对流单体。原有对流单体在原地维持成熟的结构,表现出较强的稳定性,而分裂出的新单体在移动过程中,逐渐向成熟位相发展,并且又分裂出新的单体。利用模拟结果,着重讨论了风暴发展过程中螺旋度和超螺旋度的空间结构和时间演变特征,以及在强风暴系统的对流发展过程中的动力学作用。初始环境场的螺旋性结构有利于风暴的发展。在风暴发展阶段,低螺旋度有利于大尺度向对流尺度的能量串级,而在风暴成熟阶段,高螺旋度则有利于对流单体的能量维持,从而形成长生命周期的对流系统。在风暴的发展过程中,风暴流场结构具有向Beltrami流结构的调整趋势,螺旋度向高值发展。超螺旋度在流体粘性作用的影响下,可反映出螺旋度密度空间积分的时间变化趋势,负的超螺旋度可使螺旋度增加。在对流风暴发展阶段,超螺旋度为负值,对流单体的结构螺旋性增强、螺旋度的增大,在风暴到达成熟阶段后,超螺旋度转为正值。因此,超螺旋度可用来标志对流风暴系统的成熟程度。  相似文献   
25.
该文把三维对流云模式应用于湖北省西北部地区的对流云降水研究和人工增雨试验设计,并和张家口冰雹云个例的模拟进行了比较。模拟结果表明该地区给定季节的对流云主要特征有云底温度(约26℃)。云中上升气流速度中等(最大约18m/s),初始回波在较暖区1~-2.5℃)形成,云的回波顶高约13km。前期的暖支降水对地面雨量贡献很大。播云的数值模拟结果显示了初始回波出现后约10min回波项高到达-22℃处时,在温度为-2~-6℃层的支的中心部位引进5×105~107个/kg碘化银冰核,使地面降雨只有身长弱增加。湖北西北部对流云中过冷云水偏少,最大仅5g/kg和3.8g/kg,面且过冷云水大值区温度偏高(-2.5℃).催化后云中最大上升气流和地面格点最大雨量值变化不大,有时减少,后期降雨量增加,下风方雨量增加,分布更加均匀,但总雨量增加不多。  相似文献   
26.
对流云降水过程中地形作用的数值模拟   总被引:8,自引:3,他引:8       下载免费PDF全文
该文利用地形追随坐标三维云模式,对湖北的一次对流降水过程进行了平坦地面和理想斜坡地形的模拟试验。结果发现平坦地面模拟的回波强度、最大降水强度和累积降水都与实况有相当的差距。理想地形的对流过程虽然不能模拟出对流群中多单体的生消过程,但最大降水强度和累积降水都比平坦地面的大,更接近实测结果。模拟试验表明,在地形坡度较大时,会产生较强的上升气流,从而使系统对流发展旺盛,产生较大的降水和较强的回波。所以在模拟山区和丘陵地带的对流系统时,采用地形坐标并考虑地形将会改善模式的模拟结果。  相似文献   
27.
鄂西北夏季对流降水回波特征的研究   总被引:2,自引:2,他引:2       下载免费PDF全文
该文通过对鄂西北1995~1999年6~9月273个对流回波个例进行统计分析,得出生成对流云的主要天气背景为西风低槽过境和副高外围的影响。对流云回波出现频率6、9月较少,7~8月较多。当地地形对对流云活动具有促进生成、约束移动、抬升加强等作用。对流云可分为单体、多单体、超级单体和混合云中对流等种类。6、9月对流云平均的生命时间较短,回波强度、顶高和强回波区顶高较低。相反,7~8月对流云回波特征值较高  相似文献   
28.
An equatorial β-plane model which includes realistic non-uniform land-sea contrast and the underlying surface temperature distribution is used to simulate the 30-60 day oscillation (LFO) processes in tropical atmosphere, with emphasis on its longitude-dependent evolution and convective seesaw between Indian and the western Pacific oceans.The model simulated the twice-amplification of the disturbances over Indian and the western Pacific oceans while they are travelling eastward. It reproduced the dipole structure caused by the out-of-phase oscillation of the active centres in these two areas and the periodical transition between the phases of LFO. It is suggested that the convective seesaw is the result of interaction of the internal dynamics of tropical atmosphere with the zonally non-uniform thermal forcing from underlying surface. The convective activities are suppressed over Indonesia mari-time continents whilst they are favoured over the Indian Ocean and western Pacific warm waters, so there formed two active oscillation centres. The feedback of convection with large-scale flow slows down the propagation of disturb-ances when they are intensifying over these two areas, therefore they manifest a kind of quasi-stationary component to favor the ‘dipole’ structure. Whereas the disturbances weaken and speed up over the eastern Pacific cold water re-gion due to the interaction of sensible heating and evaporation with perturbational wind. Therefore the two major centers just show out-of-phase oscillation during onecycle around the latitudinal beltBy introducing the SST anomalies in El Ni?o and La Ni?a years into the surface temperature, we also show that they have significant influence on LFO processes. In an anomalously warm year, the LFO disturbances dissipate more slowly over the central-eastern Pacific region and can travel farther eastward; whilst in an anomalously cold year, the opposite is true.  相似文献   
29.
综述了非平衡热力学应用于天气预报的若干进程以及在短期灾害性天气预报应用中的明显效果。  相似文献   
30.
1.IntroductionSouthAsiaandEastAsiaareahugemonsoonsystem,inwhichtheEastAsianmonsoonisitssubmonsoonsystem.BecausetheEastAsiansu...  相似文献   
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