一次东北冷涡中对流云带的宏微物理结构探测研究

利用2003年7月8日的东北冷涡中对流云带的飞机穿云观测资料，结合雷达、卫星云图及天气图等资料，详细分析了此次冷涡对流云带的宏观特征、微物理结构，并对降水形成机制进行初步探讨。此次东北冷涡对流云系具有明显的带状水平回波结构，中等强度，垂直尺度小（小于6 km），云过冷液态水含量丰富，最大可达3.3 g/m3，云的上部过冷水含量也达到2.0 g/m3。对流云带的上部存在冰粒子高浓度区，最大值为1062 L-1，出现在5242 m（-6.8℃） 处，这些冰粒子在高过冷水含量区的快速长大对降水产生起到重要作用。云滴直径与云滴浓度在0℃层附近呈现负相关性；通过分析解释了上升气流强的区域有更小的云滴粒子和冰晶粒子的原因，上升气流的作用造成了0℃层以下粒子浓度的积累。在弱上升气流区，2-DC观测的粒子浓度，高浓度区对应小粒子多，低浓度区对应大粒子多。并初步探讨了冷涡对流云带可能存在冰晶繁生过程。     

东亚夏季风雨带和西太平洋副高季节变化的耦合特征

利用NCEP／NCAR数据集中1950～1999年4～9月500hPa位势高度和逐日降水率(PRATE)资料，通过奇异值分解，主要探讨了东亚夏季风雨带与西太平洋副高季节移动的耦合关系。分析发现，模态方差的大小只反映模态对整个分析时段和整个分析区域贡献的大小，但对某些时段、某些区域来说，方差较小模态的贡献很大；因而仅以模态方差贡献的大小来判定模态的重要性是不完全的，只有多个模态的配合才能比较全面地揭示两个场的耦合特征。结果表明：东亚夏季风雨带在不同地区的跳跃对应着西太平洋副高的三次突变，不同模态对三次突变有不同的贡献。     

冷锋云系降水中尺度结构的一次TRMM卫星观测和特征分析

利用TRMM（the tropical rainfall measuring mission）卫星资料,对一次低槽冷锋云系和江淮气旋共同影响下的冷锋积层混合云系中雨带和雨核的特征进行了分析,研究表明,冷锋的不同部位云系结构很不均匀,可分为典型的积层混合云系、均匀的层状云系和弱的积层混合云系3种类型,南部典型的积层混合性云系中存在明显的短回波带结构,短回波带的平均长度63.0 km,宽度19.4 km,平均降雨率14.54 mm/h,同时短回波带中还有明显的雨核特征;北部均匀的层状云系中,大范围的降水在1～2 mm/h之间,其中嵌有2～7 mm/h大小不等的较强降雨带,并且存在冷锋雨带结构;中部较弱的积层混合云系中以冷锋雨带和冷锋前的暖区雨带为主,冷锋雨带上有多个雨核的结构;同时,不同性质的云系结构如短回波带、雨核以及均匀的层状云的降水的垂直廓线表现为不同的特点。     

台风利奇马登陆期间的对流结构特征及对强降雨影响

2019年9号台风利奇马在浙江造成极端降水,其中8月9日白天浙江东部受台风外围螺旋雨带长时间影响,9日夜间在台风内核对流影响下降水有显著增强;降水中心与浙江临海地区的天台山、括苍山和雁荡山等地形特征密切相关。GPM（Global Precipitation Measure）卫星遥感反演表明近岸台风螺旋雨带以层积混合型降水为主,台风眼墙区域以热带暖云对流型降水为主;眼墙区雨滴有效直径更大、雨滴数密度更高,有利于形成高降水强度。台风登陆前移动速度较慢,浙江沿海地区维持低层锋生和辐合,有利于外围螺旋雨带降水维持和增强;登陆前后受环境垂直切变等因素影响,台风中心左前侧眼墙区域对流活跃,在登陆点附近强降水区偏向于台风中心左侧。分钟级降水观测表明台风登陆期间浙江近海山区降水强度2~3倍于平原地区,其中地形性降水增幅效应与台风对流非对称结构差异对降水影响程度基本相当,有利于在台风中心左前侧的括苍山—雁荡山山区形成强降水中心。     

Impact of Cloud Microphysical Processes on the Simulation of Typhoon Rananim near Shore. Part II: Typhoon Intensity and Track

The impact of cloud microphysical processes on the simulated intensity and track of Typhoon Rananim is discussed and analyzed in the second part of this study. The results indicate that when the cooling effect due to evaporation of rain water is excluded, the simulated 36-h maximum surface wind speed of Typhoon Rananim is about 7 m s⁻¹ greater than that from all other experiments; however, the typhoon landfall location has the biggest bias of about 150 km against the control experiment. The simulated strong outer rainbands and the vertical shear of the environmental flow are unfavorable for the deepening and maintenance of the typhoon and result in its intensity loss near the landfall. It is the cloud microphysical processes that strengthen and create the outer spiral rainbands, which then increase the local convergence away from the typhoon center and prevent more moisture and energy transport to the inner core of the typhoon. The developed outer rainbands are supposed to bring dry and cold air mass from the middle troposphere to the planetary boundary layer (PBL). The other branch of the cold airflow comes from the evaporation of rain water itself in the PBL while the droplets are falling. Thus, the cut-off of the warm and moist air to the inner core and the invasion of cold and dry air to the eyewall region are expected to bring about the intensity reduction of the modeled typhoon. Therefore, the deepening and maintenance of Typhoon Rananim during its landing are better simulated through the reduction of these two kinds of model errors.     

Asymmetric rainband breaking in Typhoon Haitang (2005) before and after its landfall

Using the WRF (Weather Research Forecast) model, this work performed analysis and simulation on the rainband change during the landfall of Typhoon Haitang (2005) and found that breaking may occur over land and oceans leads to distinct asymmetric precipitation. The breaking is related to the topographic effect as well as interactions between the typhoon and midlatitude systems at upper levels. During the landfall, divergent flows at the 200-hPa level of the South-Asian high combined with divergent flows at the periphery of the typhoon to form a weak, inverted trough in the northwest part of the storm, with the mid- and low-level divergence fields on the west and northwest side of the typhoon center maintaining steadily. It intensifies the upper-level cyclonic flows, in association with positive vorticity rotating counterclockwise together with air currents that travel stepwise into a vorticity zone in the vicinity of the typhoon core, thereby forming a vorticity transfer belt in 22–25? N that extends to the eastern part of the storm. It is right here that the high-level vorticity band is subsiding so that rainfall is prevented from developing, resulting in the rainbelt breaking, which is the principal cause of asymmetric precipitation occurrence. Migrating into its outer region, the banded vorticity of Haitang at high levels causes further amplification of the cyclonic circulation in the western part and transfer of positive vorticity into the typhoon such that the rainband breaking is more distinct.     

Meridional Displacement of the East Asian Upper-tropospheric Westerly Jet and Its Relationship with the East Asian Summer Rainfall in CMIP5 Simulations

As the first leading mode of upper-tropospheric circulation in observations, the meridional displacement of the East Asian westerly jet (EAJ) varies closely with the East Asian rainfall in summer. In this study, the interannual variation of the EAJ meridional displacement and its relationship with the East Asian summer rainfall are evaluated, using the historical simulations of CMIP5 (phase 5 of the Coupled Model Intercomparison Project). The models can generally reproduce the meridional displacement of the EAJ, which is mainly manifested as the first principal mode in most of the simulations. For the relationship between the meridional displacement of the EAJ and East Asian rainfall, almost all the models depict a weaker correlation than observations and exhibit considerably large spread across the models. It is found that the discrepancy in the interannual relationship is closely related to the simulation of the climate mean state, including the climatological location of the westerly jet in Eurasia and rainfall bias in South Asia and the western North Pacific. In addition, a close relationship between the simulation discrepancy and intensity of EAJ variability is also found: the models with a stronger intensity of the EAJ meridional displacement tend to reproduce a closer interannual relationship, and vice versa.     

台风苏迪罗登陆次日分散性暴雨成因及预报着眼点

利用常规气象观测,卫星、雷达资料,数值模式和中央气象台定量降水预报数据以及FNL分析数据等对台风苏迪罗的定量降水预报进行检验,探讨台风登陆次日分散性暴雨成因和预报着眼点。苏迪罗登陆次日,暴雨分布相对较分散,各家数值模式对其把握均较差。NMC的24 h定量降水预报虽在模式基础上有较好订正,但仍存在明显的暴雨空、漏报现象:暴雨落区预报较实况偏南,导致南侧空报、北侧漏报。受环境场和台风非对称结构影响,强降水产生的有利动力、水汽条件均位于台风北侧和东部沿海地区。台风东北象限对流层低层存在两条强辐合带,其间为降水较弱的弱辐散和下沉运动区。预报员对台风结构的非对称性及风场的非均匀性把握不足,对台风中心附近和两条辐合带间的弱降水区预报偏强,造成暴雨空报。在地形作用下,浙江沿海不断有强降水产生,随后沿切线方向发展为螺旋雨带并逐渐北扩。预报员对地形不断强迫作用下降水沿螺旋雨带的发展及向外围的扩散没有预期,导致浙江北部暴雨漏报。台风登陆次日分散性暴雨的预报着眼点包括:台风非对称性、风场非均匀性、螺旋雨带发展及地形作用等。非对称性影响较大尺度的降水落区;低层风场非均匀的辐合带及急流分布则引起螺旋雨带的发展、演变,决定了台风的精细强降水落区。除地形对局地降水具有增幅作用外,强降水沿螺旋雨带的发展还会对下游地区产生影响。     

东亚春季强冷锋结构及其动力学诊断研究 II. 动力学诊断研究

在本文第I部分对东亚春季强冷锋结构进行分析的基础上，第II部分对该锋面的增强过程作了动力学诊断的研究。通过研究发现:(1)从27日08时至28日20时（北京时，下同），该冷锋处于加强阶段，锋生函数的计算显示，最大锋生区出现在对流层中层，各项的量级相同，但以倾斜项的数值为大；(2)在锋生区的南侧发现有很明显的条件对称不稳定（CSI）区域，这有利于倾斜的对流上升运动的发展，提供了一个较好的强对流系统发展的环境，对冷锋中尺度雨带的形成，CSI的激发可能有重要的作用，然而东亚春季强冷锋的CSI与北美“典型”的CSI有较明显的不同；(3)本例与Hoskins-Bretherton（HB）的理论模型所进行的比较表明，HB模型的结果可说明实际观测到的锋区的基本特征。然而，理论模型中，可能由于采用半地转假设所限，对锋后的一支下沉气流描写较弱，而这支气流对强烈天气的发展可能有重要意义。     

青藏高原热力强迫对中国东部降水和水汽输送的调制作用

从4个方面综述了有关青藏高原大地形热力“驱动”对中国东部雨带和水汽输送特征及其年代际变化的影响作用的研究进展:(1)中国三阶梯大地形热力过程变化与季风雨带季节演进;(2) 青藏高原地-气过程热力“驱动”及其季风水汽输送结构;(3) 青藏高原积雪冷源对中国东部水汽输送结构及其雨带分布的影响;(4) 青藏高原视热源变化与雨带年代际变化相关特征及其可能调制。其主要研究结论是:(1)中国西部高原特殊三阶梯大地形结构强化了海-陆热力差异,尤其是高原大地形使地-气热力差异季节变化有由青藏高原向东北方向大地形区域延伸变化趋势,且其与季风雨带由东南沿海移向西北朝青藏高原与黄土高原边缘同步演进,两者似乎存在类似季节内演进的一种“动态的吸引”。(2)中国东部雨带时空变化特征和季风强弱变化趋势均与青藏高原热源强弱异常变化相对应。青藏高原热源异常影响低纬度海洋向陆地的水汽传输路径和强度,进而调制中国东部降水时空演变。在青藏高原热源强和弱年,中国降水变率空间分布特征分别为“北涝南旱”和“南涝北旱”。青藏高原视热源强(弱)异常变化“强信号”将对东亚与南亚区域的季风水汽输送结构,以及夏季风降水时空分布的变异具有“前兆性”的指示意义。(3)长江中下游地区作为独特南北两支水汽流的汇合带,该地区夏季青藏高原热源与水汽通量相关矢特征呈类似于青藏高原多雪与少雪年水汽通量偏差场中水汽汇合区显著特征差异,揭示了冬季青藏高原积雪冷源影响中国东部夏季长江流域梅雨水汽输送结构特征。(4)中国降水的年代际变化基本型态为中国东部呈“南涝北旱趋势”,西北区域呈现出“西部转湿趋势”。但基于近10年青藏高原春季视热源出现“降后回升”趋势,中国东部“南涝北旱”的降水格局已出现转折趋势。