北京城市重烟尘雾与水雾过程的边界层结构

分析1999年11月1日至12月20日北京城市雾综合性观测试验中5次雾过程的实测资料，对如何区分重烟尘雾与水雾过程给出了判定方法，并对重烟尘雾与水雾过程的边界层结构特征作了探讨。主要结论为：从能见度、相对湿度、长波辐射平衡3个方面可以区分重烟尘雾过程和水雾过程；由于重烟尘雾和水雾的物理化学性质差异很大，对城市大气边界层结构产生的影响也不同，因此造成它们在相对湿度逆温层、风速分布、水汽变化等方面也有很大差异。     

华北平原一次大雾天气过程的数值模拟

应用非静力平衡中尺度模式MM5V3,模拟分析了2005年11月19-21日发生在华北平原的一次大雾天气过程.结果表明,本次大雾是发生在相对稳定的大气环流背景下的辐射雾.模拟的天气形势与实况基本一致,模拟雾在范围、强度、生消时间等方面基本反映了实际大雾的生消变化规律.近地层逆温的维持和充沛的水汽条件对雾层长时间维持起着重要作用.诊断分析表明,大雾维持期间,雾区近地面层处在弱的水汽辐合区;900 hPa以上为辐散区和负涡度区,整层大气中下沉运动占主导,大规模的下沉辐散运动有利于中低层大气增温,与近地层的辐射降温相配合,有助于边界层内形成逆温;冷暖平流的作用也有助于逆温形成;地面和大气的长波辐射冷却,是最主要的降温因子;太阳短波辐射是导致大雾减轻及日变化的主要原因.     

南京冬季平流雾的生消机制及边界层结构观测分析

利用系留飞艇边界层要素探测系统等设备,对2006年12月24q7日发生在南京地区的雾日边界层结构进行了综合探测,深入研究了这次平流雾的生消机制及边界层结构。结果表明：此次雾属于比较典型的平流雾,生成和维持主要决定于暖湿气流和系统性下沉运动,消散主要是干冷空气南下造成的;雾项下降阶段出现了双层结构,中层逆温是逆温主层,属于下沉逆温及平流逆温,主逆温层强中心始终位于雾顶附近或处于雾顶之下;风速随高度呈现多峰分布,中层急流与强度较弱的中上层和上层急流合并后,又与下层急流出现了一强一弱的波动;在风速较小时,风场趋于均匀化;雾消散时,低层风场趋于线性化;雾主要的水汽来源是暖湿气流;比湿场与风场有较好的时空分布对应性,主逆温层强中心也是逆湿强中心,风场与温度场共同主导了比湿场的时空分布。     

大连初冬一次辐射平流雾天气过程分析

利用大连机场地面观测资料、Micaps系统下常规资料、探空资料和NCEP/NCAR全球再分析资料,从天气形势和背景、探空资料分析和物理量诊断方面,对2009年11月30日-12月2日发生在大连地区持续性大雾天气过程做了详细分析。结果表明,本次持续性雾过程属于辐射平流雾,是在稳定的大尺度天气背景下形成的。探空资料表明,大雾发生过程中,边界层内出现一层逆温和多层逆温;边界层内近地层的逆温和充沛的水汽条件对雾的形成和长时间的维持起着重要的作用。热力结构分析表明,温度日较差大表明地面辐射冷却对本次大雾过程具有明显的作用;低层持续的弱暖平流输入,有利于近地层逆温的建立和维持。动力场结构分析表明,在中低层,大雾发生前期和维持时期,存在弱的辐合上升运动;在大雾消散期,存在明显的辐散下沉运动。水汽条件分析表明,增湿和冷却使此次大雾过程中水汽达到饱和状态产生凝结,在大雾过程的前期,存在弱的水汽辐合;在大雾消散期,存在水汽辐散。     

冀中南一次持续性大雾过程成因及维持机制

利用NCEP再分析资料、地面观测资料和微波辐射计资料,分析2019年1月11—15日河北中南部持续大雾过程的大尺度背景场、边界层特征、形成原因及维持机制等。结果表明:此次大雾产生于稳定的纬向环流背景下,其间有弱短波槽快速东移,两次干性短波槽分别促成了大雾的形成、雾区范围扩大及强度增强;大雾高度仅有几十米,以辐射雾为主,双层逆温结构为大雾的形成酝酿了先期条件,贴地逆温层内的弱水汽辐合和西南水汽输送为大雾形成和维持提供了水汽,偏北风带来的弱冷空气降温与夜间辐射降温的叠加效应是促进大雾发展的热力学条件;低层正涡度、对流层中层的辐散下沉运动是大雾维持和发展的动力因子,晴夜长波辐射和湍流混合作用促进了边界层内的降温增湿;大雾发展后期,双层逆温结构转为以单层逆温为主,最终大雾的消散主要是强冷空气入侵,大气静稳结构被破坏所致。     

环渤海近海岸雾产生的天气条件及边界层特征分析

利用渤海沿岸微波辐射计、风廓线雷达、四分量辐射仪和超声风速仪等多种观测反演资料,并结合常规站点气象资料,卫星云图,浮标气象水文观测和FNL（Final）再分析资料研究了2016年12月17~19日一次环渤海大雾个例产生的天气水文条件以及边界层垂直分层的辐射和湍流特征。研究发现:（1）此次大雾出现在大陆低压前部、入海高压后部的西南低空急流控制区域,与强急流相伴的暖湿平流输送为雾区提供了稳定的逆温和持续的水汽积累,非常有利于大雾天气的形成;（2）水汽通量的分布与低空急流的移动密切相关,近地面比湿的增速与低空急流的强度成正比;（3）由于低空急流的水汽输送增湿了环渤海低层大气,从而增强了大气辐射的衰减效应,导致雾形成前向下短波辐射逐渐减小,向下长波辐射不断增加,净辐射在大雾形成后趋近于零;（4）逆温有效抑制了湍流的发展,近地层湍流动能和摩擦速度微弱。     

华南沿海暖海雾过程中的湍流热量交换特征

湍流交换是海雾中的关键物理过程, 在海雾的热量和水汽平衡过程中起重要作用。本文根据2007年3月24～25日一次海雾的外场观测数据, 分析了海雾过程中近海面湍流热量交换特征; 并在区分风切变机械湍流与雾顶长波辐射冷却热力湍流的基础上, 着重分析了两种不同性质的湍流对海雾发展和维持的作用。结果表明: (1) 本次海雾是在西南低压和变性冷高压的控制下, 来自南海东部暖水区的空气平流在近岸冷海面上形成的暖海雾; 暖海雾中的湍流热量交换过程比冷海雾更为复杂; (2) 在暖海雾的形成和消散阶段, 风切变机械湍流的热量输送起主要作用; 而在发展和维持阶段, 既有风切变机械湍流的热量输送作用, 也有雾顶长波辐射冷却热力湍流的热量输送作用; (3) 风切变机械湍流向冷海面输送热量, 对近海面空气起到降温和增湿作用; 热力湍流同样向冷海面输送热量, 但对雾层起到增温和降湿作用; (4) 暖海雾中的湍流热量交换机制与雾层的非充分混合结构有密切关系。     

长江中上游平原地区冬季雾观测分析

长江中上游年平均雾日数达到20~106 d,是我国主要雾区之一。利用2010年12月在江汉平原观测获得的边界层廓线和雾滴谱资料,重点分析了该地区冬季雾过程的边界层结构及其生消过程。结果表明:荆州冬季雾多出现在寒潮过境1~2 d后,多为平流辐射雾;雾顶发展是水汽在上层逆温下积累,并伴随200~300 m高度冷平流降温引起;近地层冷平流降温导致饱和水汽压减小,同时上层系统性下沉增温引起逆温增强,水汽积累促使强浓雾过程产生;低空急流促使外界偏干气流与雾体混合后雾滴蒸发,是该地区雾顶迅速下降的主要原因;平均数浓度为150~406个·cm-3,极大值达到1 983个·cm-3,平均液水含量为0.014~0.118 g·m-3,极值达到0.786 g·m-3,与南京和重庆强浓雾观测值相似,超过其他地区观测值。城市地区高气溶胶浓度,配合充足的水汽条件,使得荆州雾过程微物理参量数值较大,易出现能见度小于50 m,持续时间4~9 h的强浓雾过程。     

浙江中部一次大雾过程分析与预报

利用NCEP再分析格点资料、常规观测资料、数值预报产品以及卫星云图对2009年4月6日早晨浙江中部一次大范围大雾天气过程进行诊断分析。结果表明：高空槽后暖脊的大气环流背景有利于地面长波辐射冷却和中层增温,易形成逆温,为大雾生成提供了有利条件,而边界层逆温层或等温层的形成与维持对雾的发展持续具有重要作用;凝结核、低层湍流混合是山区能见度较城镇大的主要原因;交叉温度可用来预示整个潜在雾层的湿度状态,温度与交叉温度差值可作为了解大雾生成、发展、消散过程的一项指标;模式产品能提供雾形成的环境条件;红外云图、可见光云图有助于预测雾的形成、发展、消散过程。     

江苏一次大范围的爆发性强浓雾过程研究

利用江苏省70个自动观测站和365个交通气象观测站资料,对2016年2月11日夜间至12日上午出现在江苏的一次大范围强浓雾天气过程进行分析。结果表明:这次强浓雾过程具有爆发性形成和加强的特征,大部分站点从1000m以上快速下降形成强浓雾,且部分站点存在多次爆发增强现象;夜间天空打开,长波辐射降温作用加强,是大范围强浓雾形成和爆发性发展的一个重要原因;同时,雾前降雨为本次强浓雾的形成创造了基础条件,也是日出后部分站点由于水汽蒸发增强而导致雾爆发性增强的直接原因;另外,雾前和雾期间近地层强逆温的存在为雾的爆发性发展提供了稳定的大气层结条件,而逆温顶附近低空急流的形成,也一定程度上促进了逆温的维持和加强,利于雾的爆发性发展。     

夏季青藏高原对流系统移出高原的气象背景场分析

利用1998-2004年6-8月共21个月的ISCCP对流路径集资料,结合NCEP/NCAR再分析资料和TRMM 3B42降水资料,采用合成统计分析方法,对夏季生成于青藏高原（高原）地区的对流系统进行了分类对比分析,目的在于研究各类高原对流系统动热力场的水平和垂直结构特征,探讨各类对流系统能否移出高原的气象背景场差异。结果表明,夏季高原对流系统主要生成于青藏高原中东部,存在两个高发中心。夏季高原对流系统按照对流系统的移动路径可以分为未移出高原、向南移出高原和向东移出高原3类。高原对流系统的移动、发展和生成源地没有直接关系,主要决定于气象背景场。当生成的高原对流系统上升运动强、水汽条件优越时,其强度不断增大,利于对流系统维持发展并移出高原,如果这类高原对流系统处于强西风气流控制下,容易向东移出高原,如受较强偏北风气流影响,则容易向南移出高原;而当生成的高原对流系统上升运动弱、水汽条件不理想时,其强度不断减弱,不利于对流系统发展移动,高原对流系统在高原区逐渐消亡。      

Numerical Study Of The Impact Of Coherent Structures On Vertical Transfers In The Atmospheric Boundary Layer

In two preceding papers, coherent structures of theatmospheric boundary layer (ABL), such as rollvortices or cells, were investigated through radar andaircraft observations collected during the TRAC-93(Turbulence Radar Aircraft Cells) experiment held inFrance in June 1993. The analysis of this experimentaldata set provided information on the spatialcharacteristics of these organisations (length scale,orientation, type ... ), their temporal and verticalevolution, and their relation with the dynamic andthermodynamic conditions of the ABL. For the thirdpaper in this series, a large eddy simulation model is used to examine the impact of thecoherent structures on the ABL vertical fluxes. Theanalysis of the simulated horizontal fields is madewith two-dimensional auto and cross-correlationsapplied on different pertinent ABL variables. Theresults emphasise a directional anisotropy of theseorganised fields throughout the ABL, much morepronounced in the heat flux fields, not only at thelength scale of organisations but also at theturbulence scales. This finding has an importantconsequence for traditional ABL flux measurementsbased on the hypothesis of isotropic and homogeneousturbulence. It can explain part of the underestimationof the surface fluxes often mentioned in theliterature. This approach makes it possible tomodify the concept of diffusion time (in chemicalmodelling) and could also lead to revised ABLparameterisations in Range Scale models.     

SIMULATED FINE STRUCTURES OF SPIRAL RAINBANDS IN TYPHOON CHANCHU (2006)

In this study, fine structures of spiral rainbands in super Typhoon Chanchu (2006) are examined using an Advanced Research Weather Research and Forecast (WRF-ARW) model simulation with the finest grid size of 2 km. Results show that the simulation reproduces well Typhoon Chanchu’s track, intensity and basic structures. According to their locations and features, spiral rainbands are classified into principal, secondary, inner and distant rainbands, and their dynamic and thermodynamic features are investigated. The principal rainbands remain quasi-stationary with respect to Chanchu’s center and exhibit a wavenumber-1 feature with their outer edges separated by dry air. The secondary rainbands that occur on the radially inward side of the principal rainbands move around Chanchu''s center. The inner rainbands are closest to the center. They propagate both radially outward and azimuthally with time. The distant rainbands are located outside the inner-core region, and have stronger and continuous updrafts compared to the other rainbands. Distant rainbands are inward-sloping with height along the radial direction and have a cold pool in the low layers, whereas the principal and secondary rainbands lean radially outward with height. The inner rainbands do not show tilting with height along the radial direction. However, there are few vertical tilting cells along the azimuthal orientation among the four types of rainbands. The simulated radar reflectivity cores in all rainbands are collocated with the maxima of updrafts and equivalent potential temperatures in the low layer, indicating the important roles of energy supply in the boundary layer in determining the development of the rainband convection.     

Large-Scale Motions in the Marine Atmospheric Surface Layer

Multi-level turbulent wind data from the Risø Air-Sea Experiments (RASEX) were used to examine the structure of large-scale motions in the marine atmospheric surface layer. The quadrant technique was used to identify flux events (ejections/sweeps). Ejections, which appear to occur in groups, are seen to occur first at the upper level, moving successively to lower levels with small time delays. A strong correlation between events at different heights suggests that they may all be part of a single large structure. Cross-correlation between velocity signals was used to estimate orientation of the structure using Taylor's hypothesis. The inclination of this structure is shallow ( 15°) near the surface and increases with height. Spatial representations of the fluctuating wind vectors show a structure that is strikingly similar to conceptual models of transverse vortices and shear layers seen in laboratory flows and direct numerical simulation (DNS) of low Reynolds number flows. Spatial visualization of velocity fluctuations during other time periods and conditions clearly shows the existence of shear layers, transverse vortices, plumes, and downdrafts of various sizes and strengths. A quantitative analysis shows an increase in the frequency of shear related events with increasing wind speed.     

Advanced Combination Of Spectral And Wavelet Analysis (`Spavelet' Analysis)

An advanced statistical approach named ``spavelet analysis' is described. The proposed technique combines conventional spectral and wavelet analyses to yield information about duration and periodicity of a phenomenon. The procedure consists in estimation of spectra of the wavelet coefficients at different wavelet scales. Graphic presentation of the calculated spectra in the form of a contour plot versus period and wavelet temporal scale clearly shows the predominant repetition period and durationof the analysed phenomenon. The efficiency of this technique is demonstrated using as examples both model and real atmospheric processes. This approach can have wide practical applications, being a useful tool to analyse not only atmospheric phenomena, but any kinds of random events having some certain duration and periodicity.     

中国气温涨落层次结构的区域性特征

运用近年来发展的湍流层次结构模型分析中国气温序列的涨落,研究其层次相似结构的区域性特征.通过对全国160个站点近50年来的月平均气温距平序列的分析,发现层次相似律基本上都存在,得到的层次相似系数β具有一定的区域分布特征.我们对β的含义进行了讨论,并研究了β的区域分布以及造成这种分布的原因.     

定量测量降水量的回波结构自适应算法研究

为提高临近预报中对流性降水估测的准确性,分析了统计法估算降水的局限性。依据降水物理机制和降水回波结构,研究雷达反射率因子定量测量降水量(QPE-Qualitative Precipitation Estimate)的自适应算法,旨在减少由于雨滴谱变化导致的Z-I关系不稳定所引起的降水量测量误差。同时考虑组合反射率因子RC和垂直液态水含量VIL两个参量对降水的影响,建立适于城市区域的动态自适应的Z-I关系,改进对强降水严重低估的问题。     

Tangling Turbulence and Semi-Organized Structures in Convective Boundary Layers

A new mean-field theory of turbulent convection is developed based on the idea that only the small-scale region of the spectrum is considered as turbulence, whereas its large-scale part, including both regular and semi-organized motions, is treated as the mean flow. In the shear-free regime, this theory predicts the convective wind instability, which causes the formation of large-scale semi-organized motions in the form of cells. In the presence of wind shear, the theory predicts another type of instability, which causes the formation of large-scale semi-organized structures in the form of rolls and the generation of convective-shear waves propagating perpendicular to the convective rolls. The spatial characteristics of these structures, such as the minimum size of the growing perturbations and the size of perturbations with the maximum growth rate, are determined. This theory might be useful for understanding the origin of large-scale cells and rolls observed in the convective boundary layer and laboratory turbulent convection     

台风莫拉克登陆期间的中尺度波动特征分析

利用波作用理论对台风莫拉克登陆期间的降水进行诊断分析。结果表明:波作用密度异常能在一定程度上指示暴雨雨区发展移动,其异常值的空间分布能够反映雨区上空动力场和热力场的典型垂直结构特征。台风内中尺度波动与暴雨落区宏观上具有一定联系。为了详细研究台风内部的波动特征,利用WRF(Weather Research and Forecasting model)模式模拟的高分辨率资料对台风登陆过程中波动特征进行分析,低波数波动的传播主导强对流的非对称分布,2波在登陆初期对对流分布起着关键作用,中尺度波动中同时存在涡旋罗斯贝波以及重力惯性波的特征,对登陆期间涡旋混合的现象有重要作用。     

Turbulence Over Urban-type Roughness: Deductions from Wind-tunnel Measurements

Turbulence data from experiments conducted over a staggered cube array, modelling a neutrally stable atmospheric boundary layer in an urban environment, are presented. The results support the contention that organised eddy structures in the near-wall region differ significantly from those in regular smooth-wall flows or in rough-wall boundary layers with much smaller h/δ ratios (where δ and h are the boundary-layer thickness and the height of the roughness elements, respectively). Attention is concentrated on spatial correlations, spectra (and thus the dominant length and time scales), maps of anisotropy invariants and quadrant analyses of the stress tensor. Results are obtained within both the roughness sublayer (i.e. the region above the roughness but within which the flow is spatially inhomogeneous) and the canopy region (i.e. below the height of the roughness elements) and discussion includes consideration of the turbulence kinetic energy balance at various heights.