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1.
利用多普勒雷达风廓线产品、ERA5再分析资料和WRF模式,分析了2018年6月27日皖北一次特大暴雨过程中边界层急流的日变化特征及其对特大暴雨形成的作用。结果表明:特大暴雨发生期间存在边界层急流,急流最强达到了18 m·s-1,强降水主要发生在急流快速增强的时段;急流前部的边界层辐合线是对流的触发因子,强降水落区位于急流核前部。急流为对流系统加强提供水汽和能量,且边界层急流和雷暴高压对峙使对流系统稳定少动,在对流系统西侧激发新的对流单体,有利于特大暴雨的发生;此次过程中天气系统的影响时间主要决定了强降水的落区,而边界层急流的日变化决定了强降水发生的时间段;边界层急流在夜间具有超地转特征,午后具有次地转特征,地转偏差和水平平流作用是导致夜间边界层急流增强的主要原因。  相似文献   

2.
Summary This case study describes the decay of a low-level jet in the alpine foreland as a planetary boundary layer phenomenon. Few measurements are known, which document this transition period of the boundary layer from night to day. Analysis of 1 and 20 Hz data of temperature and the three wind components of the ELECTRA aircraft mission on April 16, 1982 between 5 and 11 GMT allow an assessment of the temporal and spatial fine structure during the decay phase of the jet in the morning. Using the flight technique of horizontal and vertical zigzagging, the coupling of thermal stability, turbulence intensity, topography and behavior of the jet is shown.Vertical profiles and cross-sectional analysis of mean and turbulent parameters document three separate jet decay phases: decoupling, transition and erosion. During the first phase, the jet maximum is situated between surface and synoptic inversions, decoupling from surface friction and prohibiting momentum transport towards the free atmosphere. During the transition phase, the jet maximum increases in altitude. In the erosion phase, the jet covers the top of a developing well mixed layer. Turbulent mixing and entrainment on top of the layer are responsible for the decay of the jet. This is confirmed by calculating the decrease of the wind speed maximum from the turbulent momentum flux and the growth rate of the mixing layer by means of a mixed layer model in comparison to the measured wind speed jump and to other observations.With 7 Figures  相似文献   

3.
高空急流加速与低层锋生   总被引:27,自引:10,他引:27  
本文从动力学上找到了低层锋生函数同急流区内纬向平均风加速的关系,指出高空急流加速有利于大气低层锋生,并从天气学的角度给出了高空急流加速同低层大气锋生的环流形态特征。即高空波的动量和热量通量在急流区的辐合,促使高空急流加速,并引起急流入口区上下层之间的质量调整,在急流轴高度以下出现一个反环流,反环流的上升支同其下原有的弱锋前的上滑爬升气流发生耦合,造成上滑气流加强,低层锋面坡度变陡,冷暖对比明显,引起大气低层锋生。  相似文献   

4.
We report on observed nocturnal profiles, in which an inversion layer is located at the core of a low-level jet, bounded between two well-mixed layers. High-resolution vertical profiles were collected during a field campaign in a small plain in the Israeli desert (Negev), distant 100 km from the eastern shore of the Mediterranean Sea. During the evening hours, the synoptic flow, superposed on the late sea breeze, forms a low-level jet characterized by a maximum wind speed of 12 m s −1 at an altitude of 150 m above the ground. The strong wind shear at the jet maximum generates downward heat fluxes that act against the nocturnal ground cooling. As a result, the typical ground-based nocturnal inversion is “elevated” towards the jet centre, hence a typical early morning thermal profile is observed a few hours after sunset. Since the jet is advected into the region, its formation does not depend on the presence of a surface nocturnal inversion layer to decouple the jet from surface friction. On the contrary, here the advected low-level jet acts to hinder the formation of such an inversion. These unusual temperature and wind profiles are expected to affect near-ground dispersion processes.  相似文献   

5.
Analysis of the mean wind, equivalent potential temperature and virtual potential temperature profiles observed by the National Center for Atmospheric Research (NCAR) Electra aircraft and obtained from dropwindsondes and ship-launched radiosondes were made in conjunction with synoptic observations to study the structure of the monsoon boundary layer over the Arabian Sea during MONEX 79. Comparison of mean profiles indicates the monsoon boundary layer to be much different from the trade wind boundary layer. Results confirm the existence of a boundary-layer jet known as East African or Somali Jet. Regions of multiple cloud layers at roughly the height of the capping inversion layer were associated with the jet. Regions in which a more well-mixed layer was observed showed a jet structure depressed in height. A free-jet surface-layer model appears to describe the mean wind structure of this jet observed during the present study and by others. An approximate balance of forces was found in the monsoon boundary layer between friction, advective acceleration, Coriolis and pressure gradient forces. Friction and advective acceleration terms were significant in the lower levels of the boundary layer. Forces in a typical trade wind boundary layer were found to be approximately one order of magnitude smaller than those observed in the monsoon boundary layer.  相似文献   

6.
2020年5月22日珠江三角洲地区出现了一次极端强降水天气,最大滑动小时雨量201.8 mm,3 h雨量达到351 mm。为探讨此次极端强降水的关键预报因子及可预报性,对热带中尺度集合预报系统(CMA-TRAMS(EPS))降水预报产品进行检验评估和敏感性分析,结果表明:与欧洲中期数值预报中心集合预报系统(ECMWF-EPS)相比,CMA-TRAMS(EPS)的好成员对本次过程降水强度及位置的预报结果与实况更接近,但对极端性预报仍有欠缺。好成员的预报能力来自于对低涡和(超)低空急流的演变特征以及两者强度和位置耦合的有效预测。好成员组预报珠江三角洲东部(超)低空急流南风分量较强,有利于低涡缓慢移动和气旋性辐合增强,致使降水持续时间长、效率高。而低涡自身发展又反馈于急流强度变化,好成员组较准确地刻画了增强的低涡环流反馈导致急流小范围加速的耦合特征。其他成员组预报的低涡和(超)低空急流的耦合位置偏东、偏南,辐合强度偏弱,导致降水强度或落区出现偏差。此外,强降水致使冷池形成,并增强激烈的冷、暖气团对峙(水平温度梯度达0.23—0.76℃/km),有利于中尺度辐合线维持,加强对流后向传播并产生极端降水量。但CMA-TRAMS(EPS)两组成员在预报中尺度系统的组织性和传播特征方面均存在明显不足,限制了集合预报系统对极端降水的预报能力。   相似文献   

7.
环境场对边界层低空急流形成的影响   总被引:1,自引:1,他引:0  
本文利用两层流的浅水波模式,讨论了环境场对边界层低空急流形成的影响,并得到了边界层低空急流的特征宽度为L0=(ρ21)/(ν2ρ21ν1)L0*C0*,式中C0*=√gh2, L0*=C0*/f为Rossby变形半径,ρ1,p2和v1,v2分别为上下两层大气的密度和大尺度经向地转风,H2为低层大气的厚度,g为重力加速度,f为柯氏参数,当高低层大气中的大尺度经向地转风的垂直切变越强时,所形成的中尺度边界层低空急流就越强;当低层大气中的温度增高和湿度增大、并且低层大气中的大尺度经向地转风越强、高度越低时,越有利于形成边界层低空急流。   相似文献   

8.
登陆台风边界层风廓线特征的地基雷达观测   总被引:2,自引:0,他引:2  
为了分析登陆台风边界层风廓线特征,利用2004—2013年中国东南沿海新一代多普勒天气雷达收集的17个登陆台风资料,采用飓风速度体积分析方法,反演登陆台风的边界层风场结构特征。与探空观测对比表明,利用雷达径向风场可以准确地反演登陆台风的边界层风场结构,其风速误差小于2 m/s,风向误差小于5°。所有登陆台风合成的边界层风廓线显示,在近地层(100 m)以上,边界层风廓线存在类似急流的最大切向风,其高度均在1 km以上,显著高于大西洋观测到的飓风边界层急流高度(低于1 km)。陆地边界层内低层入流强度也明显大于过去海上观测,这主要是由陆地上摩擦增大引起。越靠近台风中心,边界层风廓线离散度越大,其中,径向风廓线比全风速以及切向风廓线离散度更大。将风廓线相对台风移动方向分为4个象限,分析边界层风廓线非对称特征显示,台风移动前侧入流层明显高于移动后侧。最大切向风位于台风移动左后侧,而台风右后侧没有显著的急流特征,与过去理想模拟的海陆差异导致的台风非对称分布特征一致。  相似文献   

9.
本文通过分析低空九层风场资料,对1987年江淮梅雨期的边界层急流的基本特征及其对梅雨过程中暴雨的动力作用做了多方面的初步研究。并与华南边支急流做了一些比较,发现江淮梅雨期的边界层急流是影响梅雨期暴雨发生与维持的一个非常重要的系统。  相似文献   

10.
采用线性化的Boussinesq流体边界层绝热流动方程,比较一维边界层急流型重力波的垂直运动量级,讨论边界层急流型重力波中的湍流发展,认为边界层急流型重力波是造成边界层飞机颠簸的一种机制。  相似文献   

11.
Four aircraft measurement sets made in late May 1989 within low level jets over the Baltic Sea have been analyzed to estimate the turbulence energy budget. It is concluded that the jets had the same origin as found in an earlier study from the same general area: inertial oscillation caused by frictional decoupling when relatively warm air flows out over much colder water.In order to combine budget estimates from the four flights to form a representative average, self-preservation similarity was assumed. When the terms were made nondimensional with the proper scale combination, the largest terms in all four runs were of order one, indicating that the scaling is physically sound.Three terms were found to dominate the turbulence energy budget: shear production, dissipation and pressure transport. The latter was obtained as remainder term, since local time rate of change and advection terms were found to be of negligible magnitude. Shear production was found in a narrow layer above the jet core and in a much deeper layer below it. The pressure transport term was a gain in this layer as well, helping to keep the layer below the jet well mixed. This is in agreement with results from aircraft measurements in the low level jet and monsoon boundary layer over the Arabian Sea.It is concluded that development of the inertial jet downwind of a coastline is of fundamental importance for exchange of momentum at the sea surface in conditions when relatively warm air is advected over cold water. The jet produces turbulence that promotes mixing in the lower layers, which sharpens the shear below the jet core, so that mixing becomes even more effective. Turbulence brought down to the surface by the pressure transport term is likely to be of the inactive type, which does not produce shear stress. Through the above-mentioned process it is, however, instrumental in promoting the mechanism that eventually produces active turbulence, the carrier of momentum.  相似文献   

12.
边界层急流型重力波——飞机颠簸的一种形成机制   总被引:4,自引:1,他引:4  
采用线性化的Boussinesq流体边界层绝热流动方程,比较一维边界层急流型重力波的垂直运动量级,讨论边界层急流型重力波中的湍流发展,认为边界层急流型重力波是造成边界层飞机颠簸的一种机制。  相似文献   

13.
北京地区夏季边界层急流的基本特征及形成机理研究   总被引:37,自引:10,他引:27  
孙继松 《大气科学》2005,29(3):445-452
首先指出了北京地区夏季边界层急流的基本特征, 即北京地区边界层急流一般出现在白天高温背景下或发生局地暴雨的夜间, 强度存在明显的日变化, 垂直分布具有明显的"鼻状"结构特征, 急流核高度一般为600~900 m.从中尺度扰动方程出发, 并通过天气过程演变实例, 研究了地形热力作用、局地强降水在边界层急流形成过程中的作用, 指出: (1)夏季高温背景下, 平原与山区之间温度梯度方向、强度的变化, 是造成低空风垂直切变加速或减速, 即边界层急流形成或消失的直接原因, 因此这种边界层急流的高度一般要低于山体的高度.(2)局地暴雨与边界层急流之间存在明显的正反馈现象: 由于局地暴雨同时改变了对流层中层和近地面层气温的水平分布, 这种热力强迫作用造成了边界层气流加速; 反过来, 边界层气流的加速又加强了急流前方的风速辐合--如果急流方向水平垂直于山坡, 这种迎风坡上的辐合将更强, 造成局地降水强度进一步增强.  相似文献   

14.
采用区域自动站逐小时降水观测数据、GPS/MET大气可降水量观测数据和NCEP/NCAR提供的FNL0.25°×0.25°分析数据,通过对比塔克拉玛干沙漠南缘和田地区2次落区接近、强度不同暴雨过程的环流和水汽特征,分析了影响极端暴雨产生的急流和水汽因子特征,结果表明:沙漠南缘暴雨时环流配置符合“三支气流”模型,高空急流、中层偏南风、低层辐合切变的强度与降水量正相关,当高层有极涡直接南伸至中亚发展而成的副热带大槽、中层有气旋前部的强偏南或西南气流、低层有偏东风急流明显西伸与西风急流形成强辐合时有利于出现极端暴雨。沙漠南缘暴雨的水汽源地、输送路径、水汽含量、饱和层厚度与降水量相关,暴雨的水汽源地一般为欧洲和北冰洋,降水区水汽输入以中低层为主,低层比湿大于6 g?kg-1,饱和层位于700 hPa以上;当中高层有来自阿拉伯海、孟加拉湾的由偏南风输送水汽的加入,低层比湿达8 g?kg-1以上、饱和层扩展至750 hPa以下时,可出现极端暴雨。  相似文献   

15.
Mixing in a two-layer stably stratified fluid by a turbulent jet was studied by a laboratory experiment. A non-swirling jet was discharged vertically downwards in a confined fluid system consisting initially of a top layer of fresh water and a bottom layer of salt water. In total, 16 experimental cases were considered, where the diameter and exit velocity of the jet were varied together with the density difference between the top and bottom layer. Vertical density profiles were determined from conductivity measurements. A three-layer density structure developed in all cases with an intermediate layer that grew in size with time elapsed as fresh and salt water were mixed. The mixing efficiency, defined as the percentage of the supplied kinetic jet energy that is used for increasing the potential energy of the fluid system, was related to a densimetric Froude number based on the intermediate layer depth. Overall, the calculated jet mixing efficiency displayed higher values than comparable efficiencies for destratification with air-bubble plumes.  相似文献   

16.
一次与西南低涡相联系的低空急流的数值研究   总被引:9,自引:0,他引:9       下载免费PDF全文
王智  高坤  翟国庆 《大气科学》2003,27(1):75-85
梅雨期西南低涡的东移发展与长江中下游降水的加强有密切关系,作者采用中尺度模式对一次西南低涡及其伴随低空急流的发展演变进行了数值模拟.模拟结果表明:在长江中下游大巴山地区低空急流先于西南涡东移发展;西南低涡及低空急流的生成发展在开始阶段与中层(400 hPa)的弱辐散密切相关;南风分量在西南低空急流的演变发展过程中起着更为主动的作用;南风分量增大中心位于南风分量中心的前方,促使南风分量中心东移;南风分量的动量方程收支分析表明水平平流项和产生项是促使南风分量变化的主要作用项,水平平流项和垂直平流项大部分相互抵消,科里奥利项的作用不可忽视,而其他项的值较小,在个别阶段和地区行星边界层项的作用在低层也较大.  相似文献   

17.
An analytical framework is proposed for studying variations in the diurnal wind structure in the planetary boundary layer (PBL) and the evolution of the low-level nocturnal jet. A time-dependent eddy-diffusivity coefficient corresponding to solar input is proposed, and an appropriate coordinate transformation ensures that mixing height varies continuously with ground heat-flux changes. The solution exhibits the receding character of the daytime PBL as evening approaches, thereby dividing the PBL into two regimes — the one just above the ground, representing the nocturnal boundary layer, and the region above it. It is assumed that inertial oscillations (IO) are triggered in the upper layer at about the time of sunset when the reversal in the direction of ground heat flux is felt in the upper layer. Two approaches are adopted to determine the characteristic features of IO and the evolution of the nocturnal low-level jet. The first one is based on the physical principle that release of horizontal momentum due to deviation from the geostrophic wind gives rise to the IO. The solution captures all the characteristic features of the IO, such as phase shift and decreasing amplitude of the IO with increasing height. According to this analysis the IO is triggered at a level as soon as the top of the receding boundary layer leaves that level. The solution is discontinuous with respect to the vertical coordinate. In the second approach we solve an initial-value problem to determine the solution in the upper layer, assuming that at about the time of sunset there is a rapid collapse of the daytime PBL to the steady, nocturnal boundary layer. The assumption is based on the mixing-height profiles prepared from climatological data collected at Delhi. The solution for the nocturnal boundary-layer regime is then obtained as a boundary-value problem. The solutions so obtained are continuous throughout the domain of interest and exhibit the characteristic features of an IO. The analysis leads to the conditions under which a low-level nocturnal jet is produced and provides quantitative estimates of the parameters, such as length of night, latitude, mixing height at sunset and nocturnal mixing height, that are conducive to the generation of a jet. The nocturnal wind profile produced by this approach compares well both with typical atmospheric data observed at Delhi and with output from a mesoscale numerical model. There is still some uncertainty related to the time of initiation of the IO as a function of latitude.  相似文献   

18.
边界层急流与北京局地强降水关系的数值研究   总被引:8,自引:0,他引:8  
应用3 km分辨率的中尺度模式,成功模拟出了2005年8月3日凌晨北京地区一次局地强降水过程,在此基础上探讨了地形热力作用和局地强降水与边界层急流的关系,结果表明,局地强降水与边界层急流之间存在正反馈作用,降水过程通过改变局地大气温度场的分布,导致边界层气流加速和急流的形成。而边界层气流的加速又加强了急流前方的风速辐合,为降水提供更多的水汽和更有利的动力条件。  相似文献   

19.
A range of large-eddy simulations, with differing free atmosphere stratification and zero or slightly positive surface heat flux, is investigated to improve understanding of the neutral and near-neutral, inversion-capped, horizontally homogeneous, barotropic atmospheric boundary layer with emphasis on the upper region. We find that an adjustment time of at least 16 h is needed for the simulated flow to reach a quasi-steady state. The boundary layer continues to grow, but at a slow rate that changes little after 8 h of simulation time. A common feature of the neutral simulations is the development of a super-geostrophic jet near the top of the boundary layer. The analytical wind-shear models included do not account for such a jet, and the best agreement with simulated wind shear is seen in cases with weak stratification above the boundary layer. Increasing the surface heat flux decreases the magnitude and vertical extent of the jet and leads to better agreement between analytical and simulated wind-speed profiles. Over a range of different inversion strengths and surface heat fluxes, we also find good agreement between the performed simulations and models of the equilibrium boundary-layer height, and of the budget of turbulent kinetic energy integrated across the boundary layer.  相似文献   

20.
2020年7月17日20时~18日20时,在淮河至长江之间出现大范围降水,短时强降水维持时间长、雨强大。此次降水发生的环流背景是:中高层多短波槽波动,伴随低层的低涡发展以及低空急流加强。强降水主要发生在低涡、切变线南侧的暖区中,降水主要分为两个阶段:第一阶段(17日20时~18日06时)强降水发生在暖式切变线和第一个低涡的暖区中,是中层潜热释放导致中层扰动形成的急流自激过程。中层位涡发展,中层扰动加强,中层扰动导致其南部急流加强,急流的自激机制形成向南、向下的上升运动波动,当水汽、能量和上升运动区配合时,形成强降水。第二阶段(18日07时~18日20时)强降水发生在第二个低涡的暖区。中高层潜热释放形成扰动,导致深厚的中低层急流发展,形成了高、中、低层一致的上升运动区。同时配合深厚低空急流带来的水汽和能量条件,形成了强降水深对流。因此整个过程的潜热释放对强降水的发展有重要作用。  相似文献   

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