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本文在已有的三维雷暴云起、放电模式中加入了一种经典的气溶胶活化参数化方案,结合一次长春雷暴个例,进行了雷暴云起放电数值模拟试验.研究显示气溶胶浓度改变对雷暴云微物理、起电及放电过程都有重要影响.结果表明:(1)污染型雷暴云中气溶胶浓度增加时,云滴数目增多,上升风速加强;云中冰晶与霰粒子数浓度增加但尺度减小;(2)相对于清洁型雷暴云,污染型雷暴云非感应起电过程弱,感应起电过程强,起电持续时间长;(3)污染型雷暴云中首次放电时间延迟,闪电持续发生的时间长,总闪电频次增加,正地闪频次增加明显. 相似文献
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本研究利用加入起电、放电参数化方案的数值模式（Weather Research and Forecasting Model（Version 3.7.1）,WRF3.7.1_ELEC）,通过设计五组不同非感应起电及感应起电参数化方案敏感性试验,对发生在青藏高原东北部青海大通地区的一次雷暴过程进行模拟研究,对比分析了不同非感应起电机制及感应起电机制对雷暴云电荷结构的影响.结果表明：在雷暴云发展旺盛阶段,Saunders（S91）、Riming Rate（RR）、和Saunders和Peck（SP98）三种非感应起电方案模拟的雷暴云最低层均为负电荷区,而混合方案（Brooks and SP98,BSP）模拟的雷暴云最低层为正电荷区,主电荷区自下而上为"+-+-"排列的四层电荷结构.与甚高频辐射源定位法推算的结果对比,BSP方案模拟的本次高原雷暴云电荷结构更接近实际情况;几种不同非感应起电方案模拟的主电荷区外围与主电荷区电荷结构不同,说明在雷暴发展的不同阶段雷暴云的电荷结构是不同的;几种非感应起电方案模拟的电荷结构不尽相同,主要是由于霰、冰和雪粒子在不同高度所带电荷的极性及电量的大小不同,霰粒子的电荷密度对低层的影响较大,冰粒子和雪粒子的电荷密度对中上层的影响较大;加入感应起电机制后,雷暴云电荷结构分布几乎没有变化,但能使雷暴云发展旺盛阶段低层和中层的正负电荷区电荷密度有所加强. 相似文献
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我们应用改进的随机闪电参数化方案，对两次雷暴的起、放电过程进行了二维125 m和250 m分辨率云闪模拟试验，分析表明高分辨率模拟的云闪通道几何结构、延伸范围和最大垂直电场变化等特征与观测结果更为一致，并且揭示了云闪放电重新配置云内电荷分布和空间电荷中和过程的一种新的物理图像：(1) 云闪的直接物理效应是在已有的空间电荷区内沿着放电通道沉积异极性电荷、形成复杂的空间电荷分布，有效地导致云中电位和场强绝对值及静电场能量剧烈下降，使放电终止.其中：放电后在闪电通道经过主要区域，电位降到±30 MV之间，垂直电场强度也降到±20 kV·m-1之间，一次正或负云闪估计消耗掉107～1010 J静电能；(2) 云中电荷中和不是正、负空间电荷简单地直接相互抵消的瞬态过程，而是广泛分布的云中空间电荷与通道沉积的异极性电荷通过湍流交换、平流输送、重力沉降以及起电等多种因素逐渐混合并部分被中和的一个后续慢过程，其弛豫时间典型值在14～44 s之间，在此期间通道感应电荷总量下降到50%以下.并残余部分电荷参与后续放电前高空间电荷密度和强电场的重建过程. 相似文献
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本文针对中国暴雨发生发展天气特征,改进和发展了一种适合于描述东亚暴雨的中尺度积云参数化方案.首先基于近年来(1990—2010)江淮流域汛期降水合成分析的基础上,诊断出组织化对流降水环境的动力参数;其次利用该动力参数作为动力控制条件,改进了Kain-Fritsch Eta中尺度积云对流参数化方案;最后利用改进的中尺度积云参数化方案对梅雨期暴雨、华南前汛期暴雨过程进行了数值模拟,结果表明:改进后的中尺度积云参数化方案对上述两次暴雨过程的落区及强度的模拟,均有明显改进. 相似文献
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积云对流参数化方案对热带大气季节内振荡模拟的影响 总被引：2，自引：0，他引：2
本文利用中国科学院大气物理研究所大气科学和地球流体力学数值模拟国家重点实验室（LASG）的大气环流谱模式的最新版本SAMIL2.2.3系统分析了积云对流参数化方案对热带大气季节内振荡（ISO）模拟的影响.结果表明该模式的三种积云对流参数化方案都能模拟出热带地区气候平均季节内振荡（CISO）时空演变的基本特征;其中Tiedtke方案相比于Manabe方案和Zhang-McFarlane方案,模拟出的CISO与观测更为接近.而SAMIL2.2.3模式对ISO年际变化部分（TISO）的模拟结果显示尽管SAMIL2.2.3相对于之前的版本对Tiedtke方案和Zhang-McFarlane方案针对不同问题做了必要调整,但三种积云参数化方案中只有Zhang-McFarlane方案能够模拟出27～50天TISO模态的东传特征.另外,SAMIL2.2.3与其较早版本SAMIL2.08中的Manabe方案完全相同,物理过程的其他部分如辐射方案和气溶胶条件有所调整,但仅后者能模拟出100E以西热带27～50天TISO模态的东传特征.因此,模式发展过程中物理参数化方案的改进并非在每一方面上都产生正面效果.动力框架和物理过程,以及不同物理过程之间的协调发展是改进模式的重要途径. 相似文献
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随着空基、地基云状观测自动化进程的推进,国际通用的人工观测云分类标准不再适用于自动观测.本文提出了适用于自动观测的卫星观测、地基观测和数值预报模式统一的云分类原则和分类标准,依据大气代表性原则、仪器观测可行性原则、历史继承性原则和可扩展性原则,不考虑云的高度,沿用形态学和发生学理论,将云分为卷云、层状云、波状云和积状云4属,更细分为薄卷云、密卷云、波云、雨波云、层云、雨层云、浅积云和深积云8类,列出了各类云特征的定性描述,为自动观测、预报保障和模式评估提供参考. 相似文献
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国内外大地电场观测及其地震预报研究综述阮爱国（国家地震局兰州地震研究所兰州７３００００）大地电场观测和研究是地震预报中新发展的一种前兆手段，它来自于地球物理勘探中的地电场法，但又不同于后者。它以孕震过程中的电现象为研究对象，研究地球自身感应电场在地球... 相似文献
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利用数值模拟的方法，研究了雷暴放电后，由雷暴电荷、感应电荷和晴天大气的背景电荷共同产生的准静电场(Quasi electrostatic field, 简称QEF)的时变过程，以及准静电场对中性大气的加热和电离. 结果表明: 在考虑电离层电势和晴天大气背景电场的影响后，时变的准三维的准静电场（QEF）模式能较好地解释“红闪”(Red sprites)的时空特征，特别是能模拟出“红闪”中的一种——“闪晕”（sprite halo）向上弯曲的空间结构. 相似文献
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2.1地震孕育和发生过程中的电异常现象
2.1.1地电场及震前地电场异常.地球表面存在着天然的变化电场和稳定电场,天然变化电场的大部分是由地球外部各种电流系在地球内部感应产生的,分布于整个地表的广大地区,一般具有较小的梯度;另外还有一小部分是由于地球内部的某些地球物理、化学变化产生的,出现在某些特定的时间和区域,一般也具有较小的梯度变化,但有时可能引起较大的电位梯度变化. 相似文献
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The inverted charge structure formation of a hailstorm was investigated using the Advanced Weather Research and Forecasting(WRF-ARW) model coupled with electrification and discharge schemes. Different processes may be responsible for inverted charge structure in different storms and regions. A dynamical-derived mechanism of inverted charge structure formation was confirmed by the numerical model: the inverted structure was formed by strong updraft and downdraft under normal-polarity charging conditions such that the graupel charged negatively in the main charging region in the middle-upper level of the cloud. The simulation results showed the storm presented a normal charge structure before and after hail-fall; while during the hail-fall stage, it showed an inverted charge structure—negative charge region in the upper level of the cloud and a positive charge region in the middle level of the cloud—appearing at the front edge near the strong updraft in the hailstorm. The charging processes between the two particles mainly occurred at the top of the cloud, where the graupel charged negatively and ice crystals positively due to the strong updraft. When the updraft air reached the top of the storm, it would spread to the rear and front. The light ice crystals were transported backward and forward more easily. Meanwhile, the positively charged ice crystals were transported downward by the frontal subsidence, and then a positive charge region formed between the ?10 and ?25°C levels. Subsequently, a negative charge region materialized in the upper level of the cloud, and the inverted charge structure formed. 相似文献
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FengXia Guo GanYi Lu Xin Wu HaoLiang Wang ZuPei Liu Min Bao YaWen Li 《中国科学:地球科学(英文版)》2016,59(7):1401-1413
The purpose of this study was to understand the reasons why frequent positive cloud-to-ground (+CG) flashes occur in severe thunderstorms. A three-dimensional dynamics-electrification coupled model was used to simulate a severe thunderstorm to permit analysis of the conditions that might easily cause +CG flashes. The results showed that strong updrafts play an important role in the occurrence of intracloud flashes. However, frequent +CG flashes require not only strong updrafts but also strong downdrafts in the lower cloud region, conditions that correspond to the later phase of the mature stage and the period of the heaviest solid precipitation of a thunderstorm. During this stage, strong updrafts elevated each charge area in the updraft region to a higher level, which resulted in an inverted tripole charge structure. A wide mid-level region of strong positive charge caused largely by positively charged graupel, presented in the middle of the updraft region because of a non-inductive ice-ice collisional charging mechanism. The charge structure in the downdraft region was consistently more complex and revealed several vertically stacked charge regions, alternating in polarity. Much of the graupel/hail outside the updrafts was lowered to cloud-base by strong downdrafts. In this area, the graupel/hail was charged negatively because of the transportation of negatively charged graupel/hail from higher regions of negative charge in the updrafts, and via the inductive charging mechanism of collisions between graupel/hail and cloud droplets at the bottom of the cloud. Consequently, a large region of negative charge formed near the ground. This meant that +CG flashes were initiated more easily in the lower inverted dipole, i.e., the middle region of positive charge and lower region of negative charge. Frequent +CG flashes began almost synchronously with dramatic increases in the storm updrafts, hail volume, and total flash rate. Therefore, the occurrence of +CG flashes appears a good indicator of storm intensification and it could have some use as a predictor of severe weather in the form of hail. 相似文献
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Recondensed meteoric material, so-called meteoric smoke, has long been considered the main candidate for condensation nuclei for mesospheric ice formation. Recently however, model studies have shown that meteoric smoke particles are transported away from the polar region, where ice phenomena such as noctilucent clouds occur, before they can grow large enough to serve as ice condensation nuclei. In the accompanying paper it is argued that charging of the meteoric smoke particles may solve this dilemma by significantly altering the efficiency of the particles as condensation nuclei. In the present paper, the feasibility of this idea is investigated more quantitatively, by analysing the time scales of processes such as charging, recombination, and particle growth. Despite large uncertainties, especially in the charging efficiency of the smallest smoke particles, we show that reasonable assumptions yield number densities of charged condensation nuclei that are consistent with what is expected for mesospheric ice phenomena. 相似文献
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This paper proposes a new model for thunderstorm electric field generation which directly utilizes the dynamic turbulent motion to separate the charges. Postulating a microphysical charge separation mechanism, such as is commonly accepted in most other theories, and which places a negative charge on the larger particles with a positive charge on the smaller ones, it is described how evaporation and cooling at the tops of small cumuli will release the positive charges as ions. These ions migrate to the surrounding cloud as the cooled parcel, with negatively charged particles in it, sinks down through the cloud. Since the sinking parcel contains mostly ice, it will be more buoyant than its surroundings when it reaches rising regions of water cloud, and hence should come to rest near the –10°C level. Thus the cloud will acquire an accumulation of negative charge at about this level before substantial hydrometeors begin falling out of it. 相似文献
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In this study, the formation of a contrail from an aircraft flying near the tropopause is simulated using a three-dimensional mesoscale atmospheric model including a very complex scheme of parameterized cloud microphysical processes. Two different primary ice nucleation parameterizations for deposition nucleation, condensation freezing, and contact freezing are applied. The model-predicted ice concentrations are compared to data measured during the International Cirrus Experiment (ICE), 1989. 相似文献
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B. Strauss R. Meerkoetter B. Wissinger P. Wendling M. Hess 《Annales Geophysicae》1997,15(11):1457-1467
The impact of contrail-induced cirrus clouds on regional climate is estimated for mean atmospheric conditions of southern Germany in the months of July and October. This is done by use of a regionalized one-dimensional radiative convective model (RCM). The influence of an increased ice cloud cover is studied by comparing RCM results representing climatological values with a modified case. In order to study the sensitivity of this effect on the radiative characteristics of the ice cloud, two types of additional ice clouds were modelled: cirrus and contrails, the latter cloud type containing a higher number of smaller and less of the larger cloud particles. Ice cloud parameters are calculated on the basis of a particle size distribution which covers the range from 2 to 2000 m, taking into consideration recent measurements which show a remarkable amount of particles smaller than 20 m. It turns out that a 10% increase in ice cloud cover leads to a surface temperature increase in the order of 1K, ranging from 1.1 to 1.2K in July and from 0.8 to 0.9K in October depending on the radiative characteristics of the air-traffic-induced ice clouds. Modelling the current contrail cloud cover which is near 0.5% over Europe yields a surface temperature increase in the order of 0.05 K. 相似文献