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1.
气溶胶、云、降水相互关系是现今大气科学的前沿领域。本文总体概括了气溶胶作为云凝结核和冰核,对云宏微观物理特性及降水的影响原理研究的主要成果。并根据气溶胶自身化学性质的吸湿性,从吸湿性气溶胶和非吸湿性气溶胶两方面,重点探讨了模拟研究中,硫酸盐、海盐、沙尘、黑碳气溶胶对于云和降水的影响,以及各类气溶胶与其它类型气溶胶相比,作用于云降水的不同方式。提出之前研究工作的不足,以期为今后该方向的研究提供一些思路。   相似文献   

2.
3.
沙尘气溶胶对云和降水影响的模拟研究   总被引:9,自引:0,他引:9  
采用二维分档云模式,对比背景大气气溶胶分布,讨论了扬沙和沙尘暴天气条件下矿物气溶胶对云微物理结构、光学特性以及降水形成的影响.结果表明:扬沙和沙尘暴天气增加大气中大核和巨核的浓度,促进云中水汽的活化,使降水提前出现,暖云和冷云降水量均大幅增加,但可忽略巨核增加对云光学厚度和反照率的作用;当矿物沙尘粒子同时作为有效的云凝结核和冰核参与云的发展时,冰核浓度增加使水成物有效半径减小,抑制了暖云和冷云降水,云内存留的大量冰晶增强云的光学厚度和反照率.  相似文献   

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5.
气溶胶直接效应对一次降水影响的机理分析   总被引:2,自引:0,他引:2  
利用完全在线耦合气溶胶-辐射-云-降水相互作用的WRF-Chem模式研究了气溶胶直接效应对2012年7月21日一次暴雨的影响。结果表明,WRF-Chem模式较好模拟了此次降水过程中气象场和化学场的变化;模式基本模拟出此次降水的发展过程和总降水量的空间分布特征,气溶胶直接效应不会改变整体降水强度和区域总降水量,但会改变区域内的降水分布形态。在污染地区吸收性气溶胶对太阳短波辐射的吸收使大气中层加热,增强了相应大气层之间的不稳定性,使垂直运动更加强盛,由此霰和雨水对云水的收集增强,可降水粒子增加,降水增强;相反,在污染地区的下风向动力过程则相对减弱,降水减少。气溶胶直接效应通过影响动力过程和微物理过程改变降水的分布   相似文献   

6.
飞机观测是云中粒子相态、分布和转化特征的重要探测技术。我国云降水物理飞机观测开始于20世纪60年代,经过60多年的发展,在飞机平台、机载测量技术、云微物理结构和降水形成机制认识等方面均取得了长足进步。发现积层混合云中对流泡区具有更高的过冷水含量,凇附增长起重要作用,符合“播撒-供给”降水形成机制,而在层云区,当云厚度较小时,过冷水含量很少,冰雪晶的凝华、聚并增长起主导作用,并不符合“播撒-供给”降水形成机制,而当云厚度较大时,过冷水含量较为丰富,凝华、聚并和凇附增长起主导作用,基本符合“播撒-供给”降水形成机制;我国北方冬季降雪过程的形成机制主要是凝华-聚并机制,只有在水汽非常充足、云较厚的情况下,凇附增长过程才具有重要作用。近年虽然在人工影响天气播撒效应、数值模式云物理过程验证、卫星及雷达遥感数据检验、对流云结构观测等方面也取得了一些进展,但仍较薄弱,亟待加强。  相似文献   

7.
云和气溶胶对温度影响的初步研究   总被引:1,自引:0,他引:1  
  相似文献   

8.
中国北方沙尘气溶胶对云和降水影响的数值模拟研究   总被引:2,自引:2,他引:2  
康凤琴  银燕  张逸轩 《气象》2009,35(6):36-45
已有的研究表明中国北方千旱半干旱地区是对流层沙尘气溶胶的主要来源之一,对当地乃至全球气候都有重要的意义.利用数值模拟研究方法探讨不同干燥程度的大气背景环境下,沙尘气溶胶数浓度对混合云形成和发展的可能影响,并采用析因试验讨论了主次影响因素.结果表明:沙尘气溶胶的增加导致降水减少、延长了云在空中存在的时间,改变了云的空间结构和微观结构.析因分析表明干旱半干旱气候背景条件下,混合云的累计降水量对沙尘气溶胶数浓度变化的敏感性要高于对大气环境湿度的敏感性;沙尘气溶胶数浓度增加导致云累计降水量的减少;沙尘气溶胶数浓度和大气环境湿度对云的累计降水量的影响是复杂的,研究结果可以用于指导降水预报业务.  相似文献   

9.
青藏高原(简称高原)气溶胶主要来自周边地区的输送,近年来,随着人为污染加剧和气候条件变化,高原及周边地区气溶胶的特性和气候效应越来越受关注。而高原降水一直是高原气象与气候学的重点,气溶胶对高原降水的影响正逐渐成为研究热点。本文总结了高原气溶胶及其对降水影响的相关研究成果,从气溶胶特性观测(站点和卫星观测)研究、“气溶胶-辐射相互作用”、“气溶胶-云相互作用” 影响降水研究以及气溶胶影响降水中化学组分研究等方面进行了综述,并对未来研究方向进行了展望。  相似文献   

10.
气溶胶影响混合相对流云降水的数值模拟研究   总被引:2,自引:0,他引:2  
利用一种新的异质冰相核化参数化方案,研究了当气溶胶同时作为云凝结核和冰核时,在不同高度输送对混合相对流云和降水的影响。结果发现,对于本文研究的理想混合相对流云,气溶胶在边界层的输送导致液滴数浓度明显增加,有效半径减小,霰粒的生长受到抑制,引起霰粒质量浓度降低;而气溶胶在对流层中层4~6km输送时,导致冰晶和霰粒数浓度明显增加。由于较多的冰晶引起更加快速的贝吉隆过程,使霰粒的质量浓度增加;气溶胶在对流层中层2~4km高度输送时冰相形成作用相对较弱,并引起霰粒的数浓度略微增加,由于霰粒的有效半径减小导致其质量浓度下降。气溶胶在不同高度的输送都导致液态和固态降水率降低,随着背景气溶胶数浓度的增加,气溶胶在0~2km、2~4km以及4~6km的输送分别导致累积降水量减少28%~64%、4%~44%和3%~46%,并且对降水的抑制效应及所在高度不同引起的降水差异随着背景气溶胶数浓度的增加而减小。  相似文献   

11.
气溶胶对北京中尺度对流系统影响的数值试验   总被引:2,自引:5,他引:2  
利用可分辨云模式(WRF),模拟研究了不同气溶胶浓度对北京地区2001年8月23日一次产生强降水和冰雹的对流天气的影响。结果表明,气溶胶浓度的增加不利于对流云的发展,导致地面降水减小,但是对降水结构没有明显影响。气溶胶浓度增加导致云中水成物数浓度和质量浓度均发生变化,其中云水、冰晶和雪含量增加,而雨水、霰和雹含量减小。从云微物理学分析发现,气溶胶浓度减小有利于高层云的形成,云滴有效半径随着气溶胶浓度增加而减小。  相似文献   

12.
利用WRF v3.6.1模式,采用Thompson云微物理参数化方案对北京奥运会期间的一次降水过程进行了模拟,通过3组数值试验对比分析了高、中、低云凝结核浓度对降水的影响。数值试验结果显示:(1)在云凝结核浓度较低的情况下,云凝结核浓度增加使24 h累积降水量增加,且增加的幅度相对较低;在云凝结浓度较高的情况下,云凝结核浓度增加使24 h累积降水量减少,且减少的幅度相对较高。(2)从地面雨强分布来看,不同的云凝结核浓度对暴雨、大雨、中雨、小雨的影响均体现在降水强度上,对降水位相的影响不显著。(3)云凝结核浓度的变化对低云量的影响与其对降水的影响相一致,故低云量是影响降水的一个重要因素。  相似文献   

13.
利用2006—2016年夏季中分辨率成像光谱仪(Moderate-resolution Imaging Spectroradiometer,MODIS)气溶胶和云资料以及热带降水测量计划(Tropical Rainfall Measuring Mission,TRMM)降水数据,分析了中国8个典型地区气溶胶、云和降水的时空分布特征,探讨了气溶胶与云和降水的相互关系。结果表明:中国8个典型地区夏季平均气溶胶光学厚度(Aerosol Optical Depth,AOD)、云光学厚度(Cloud Optical Depth,COD)、云水路径(Cloud Water Path,CWP)、水云云滴有效粒子半径(Cloud Effective Radius Water,CERW)、冰云云滴有效粒子半径(Cloud Effective Radius Ice,CERI)和降水强度变化范围分别为0.21—1.05、15.01—24.02、151.98—219.20 g·m-2、12.93—15.37 μm、28.85—39.14 μm和0.44—8.54 mm·d-1;黄土高原和四川盆地AOD有显著降低趋势,年倾向分别为-2.30%和-3.20%,长江三角洲COD年增幅为29.11%,华北平原、长江三角洲和珠江三角洲CERI及塔克拉玛干沙漠CERW变化趋势分别为-21.60%、-15.77%、-18.94%和-10.31%;AOD与COD和CWP呈正相关,与云滴有效粒子半径(Cloud Effective Radius,CER)关系较为复杂,受水汽影响较大,在云层含水量较低的情况下,CERI(CERW)与AOD呈负(正)相关,而在云层含水量较高的情况下,二者呈正(负)相关;气溶胶和降水关系复杂,整体来看,气溶胶促进了中国地区的夏季降水。  相似文献   

14.
The effect of clouds on aerosol growth in the rural atmosphere   总被引:1,自引:0,他引:1  
Measurements of accumulation mode aerosol in the atmospheric boundary layer under cloudy and cloud-free conditions, and in the lower free troposphere under cloud-free conditions, were conducted over the rural northwest of England. Normalised size distributions in the cloud-free boundary layer (CFBL) and the cloud-free free troposphere (CFFT) exhibited almost identical spectral similarities with both size distributions possessing a concentration peak mode-radius of ≈0.05 μm or less. By comparison, aerosol distributions observed in cloudy air exhibited a distinctive log-normal distribution with mode-radii occurring at ≈0.1 μm concomitant with a local minimum at ≈0.05 μm. The consistent and noticeable difference in spectral features observed between cloudy and cloud-free conditions suggest that a greater amount of gas-to-particle conversion occurs on cloudy days, presumably through in-cloud aqueous phase oxidation processes, leading to larger sized accumulation mode particles. Apart from the distinct difference between cloudy and cloud-free aerosol spectra on cloudy days, aerosol concentration and mass were observed to be significantly enhanced above that of the ambient background in the vicinity of clouds. Volatility analysis during one case of cloud processing indicated an increase in the relative contribution of aerosol mass volatile at temperatures characteristic of sulphuric acid, along with a smaller fraction of more volatile material (possibly nitric acid and/or organic aerosol). Growth-law analysis of possible growth mechanisms point to aqueous phase oxidation of aerosol precursors in cloud droplets as being the only feasible mechanism capable of producing the observed growth. The effect of cloud processing is to alter the cloud condensation nuclei (CCN) supersaturation spectrum in a manner which increases the availability of CCN at lower cloud supersaturations.  相似文献   

15.
A model of the aqueous phase processing of an aerosol population undergoing multiple cycling through a stratocumulus (Sc) cloud layer is presented. Results indicate that a significant modification of the aerosol properties is achieved following the first cycle through cloud. In a polluted atmosphere, further modification in subsequent cycles is seen to be hydrogen peroxide limited unless there is a flux of ammonia entering the system through cloud base (CB). The modification of the aerosol population is seen to have little effect on the microphysics (specifically the cloud droplet concentration and effective radius) of the processing cloud. However, it enables processed aerosols to subsequently act as efficient cloud condensation nuclei (CCN) in less vigorous clouds (as a result of reducing the critical supersaturation required to activate them). The effects of variations in the internal mixture of soluble components of aerosols on the microphysics of clouds forming on them are also investigated using the cloud model. A (K2) parameterisation of the effects of variations in internally mixed nitrate loadings on the cloud droplet number concentration is presented. The effects of applying this K2 correction to the droplet number (derived from a parameterisation based on sulphate) for the presence of nitrate in aerosol have been investigated using the HadAM3 version of the Hadley Centre General Circulation Model (GCM). The effect on global annual mean simulations of the indirect forcing and effective radius is small, but more pronounced regionally. Suggestions (based on model results and observations) for parameterising the size distribution and in-cloud growth of aerosols for use in GCMs are presented.  相似文献   

16.
In this study, linkage between changing characteristics of precipitation extremes and cloud covers over Central India is explored during summer monsoon period using Satellite data (1998–2015). This is a first attempt to relate the changes in cloud cover to the changes in precipitation extremes. Non-rainy cirrus clouds are excluded from this study. Results show that heavy rainfall (≥ 60 mm/day) is associated with cold cloud tops (Tb≤220 K) while moderate rainfall (<60 mm/day and ≥20 mm) occurs mostly with middle clouds (Tb>220 K and ≤245 K). Low level clouds (Tb> 245 K) are responsible for light rainfall (<20 mm/day). Increases in top 20%, 10%, 5% and 1% heavy precipitation relate well with the increases in very deep convective, deep convective and convective cloud cover. Among these relations, increase in top 5% heavy precipitation relates best with increase in very deep convective cloud cover. Decrease in bottom 30% low precipitation relates with decrease in low level cloud cover. The results reported in this study fit into the framework of how weather extremes respond to climate change.  相似文献   

17.
东亚季风气候受到自然因素和人类活动的共同影响,而人类活动因子中气溶胶的作用尤为关键,采用诊断分析的手段研究东亚地区气溶胶的特征及其与云和降水的相互关系具有重要的科学意义。本文利用MODIS(moderate-resolution imaging spectroradiometer)气溶胶和云资料以及TRMM(Tropical Rainfall Measuring Mission)降水数据,分析了东亚夏季气溶胶、云、降水的时空分布特征,研究了气溶胶与云和降水的相互关系。结果表明:中国四个典型地区(珠三角、长三角、四川盆地、京津唐)2001~2011年夏季(6~8月)平均气溶胶光学厚度(Aerosol Optical Depth, AOD)变化范围为0.40~0.68,云光学厚度平均值为18.7~23.6,水云云滴有效粒子半径在20.2~25.6 μm,冰云有效粒子半径在12.9~15.3 μm,云水路径为222.2~243.8 g m-2,降水强度平均值3.6~8.6 mm d-1;珠三角气溶胶光学厚度有显著降低趋势,年倾向为-3.31%,四川盆地云滴有效粒子半径(冰云、水云)和云水路径年变化趋势为-0.42%、-0.49%和-1.26%,京津唐夏季降水量年增幅为3.24%。气溶胶光学厚度和云光学厚度呈正相关,相关系数最大为0.77;在相对湿度较低(30%~50%)情况下,气溶胶光学厚度与云滴有效粒子半径呈负相关;气溶胶光学厚度与云水路径呈正相关,相关系数最大为0.92;相对于低污染情况(AOD<0.5),高污染情况(AOD>0.5)下出现大雨(>10 mm d-1)的频率增加了6.6%~19.1%,小雨(<1 mm d-1)的频率减少了0.72%~7.3%。在水汽含量较少的情况下,气溶胶的增加导致云滴有效粒子半径的减少;气溶胶增强了南方地区的对流性降水,抑制了北方地区层云降水。  相似文献   

18.
城市化对广州降水的影响分析   总被引:7,自引:1,他引:7  
利用1959—2009年逐日降水观测数据,分析了广州51 a来降水的变化规律。发现城郊增城年总降水量变化趋势不明显,但大暴雨降水日数有所增加;广州年降水总量总体呈波动变化,1991年以来有微弱的增加趋势,增率为105 mm/a。而从降水等级日数和降水负荷上分析发现,1982年以来,广州年降水日数有下降的趋势,减少率为72 d/10a;而1991年以来,广州大雨以上等级降水日数和降水负荷均有明显的上升趋势,其中大雨降水日数增长率为28 d/10a,暴雨降水负荷增长率为24%/10a;城市化造成了广州大雨、暴雨和大暴雨等年强降水日数增加,相比1960—1979年,分别增加了6%、11%和23%;相对于城市化之前,从1991年开始,城市化过程使得广州降水量增加的趋势明显,城市化对广州城市降水增加的贡献率为447%。  相似文献   

19.
一次秋季冷锋降水过程气溶胶与云粒子分布的飞机观测   总被引:1,自引:1,他引:1  
利用机载PMS(Particle Measuring Systems)测量系统,对2008年10月4—5日石家庄地区一次冷锋降水云系的3次气溶胶和云粒子探测资料进行了分析。结果表明,冷锋过境降水前后,气溶胶粒子分布差异较大。降水发生前,气溶胶粒子平均数浓度约为103cm-3,平均直径为0.95μm;气溶胶主要集中于3000m高度以下的对流层低层,云内气溶胶数浓度明显减少。降水发生后,气溶胶粒子平均数浓度约为102cm-3,比降水前约小1个量级,平均直径为1.28μm;气溶胶主要集中于1200m以下的近地面层,其数浓度随高度增加而降低。气溶胶粒子浓度在低层云区内水平变化较小,而在无云区和云下近地层水平起伏较大。云粒子平均浓度比气溶胶小1~2个量级。气溶胶粒子平均谱主要呈双峰型,而云粒子谱主要为单峰型。  相似文献   

20.
A two-dimensional cloud model with bin microphysics was used to investigate the effects of cloud condensation nuclei (CCN) concentrations and thermodynamic conditions on convective cloud and precipitation developments. Two different initial cloud droplet spectra were prescribed based on the total CCN concentrations of maritime (300 cm− 3) and continental (1000 cm− 3) air masses, and the model was run on eight thermodynamic conditions obtained from observational soundings. Six-hourly sounding data and 1-hourly precipitation data from two nearby weather stations in Korea were analyzed for the year 2002 to provide some observational support for the model results.For one small Convective Available Potential Energy (CAPE) ( 300 J kg− 1) sounding, the maritime and continental differences were incomparably large. The crucial difference was the production of ice phase hydrometeors in the maritime cloud and only water drops in the continental cloud. Ice phase hydrometeors and intrinsically large cloud drops of the maritime cloud eventually lead to significant precipitation. Meanwhile negligible precipitation developed from the continental cloud. For the three other small CAPE soundings, generally weak convective clouds developed but the maritime and continental clouds were of the same phases (both warm or both cold) and their differences were relatively small.Model runs with the four large CAPE ( 3000 J kg− 1) soundings demonstrated that the depth between the freezing level (FL) and the lifting condensation level (LCL) was crucial to determine whether a cloud becomes a cold cloud or not, which in turn was found to be a crucial factor to enhance cloud invigoration with the additional supply of freezing latent heat. For two large CAPE soundings, FL–LCL was so deep that penetration of FL was prohibitive, and precipitation was only mild in the maritime clouds and negligible in the continental clouds. Two other soundings of similarly large CAPE had small FL–LCL, and both the maritime and continental clouds became cold clouds. Precipitation was strong for both but much more so in the maritime clouds, while the maximum updraft velocity and the cloud top were slightly higher in continental clouds. Although limited to small CAPE cases, more precipitation for smaller FL–LCL for a selected group of precipitation and thermodynamic sounding data from Korea was in support of these model results in its tendency.These results clearly demonstrated that the CCN effects on cloud and precipitation developments critically depended on the given thermodynamic conditions and not just the CAPE but the entire structure of the thermodynamic profiles had to be taken into account.  相似文献   

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