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1.
贺兰山地区沙尘气溶胶瞬时谱分析及拟合   总被引:3,自引:2,他引:3  
利用APS-3310A型激光空气动力学粒子谱仪,1998年4、5月和1999年4月在贺兰山附近的巴音浩特、盐池、银川等地采集了具有代表性的背景大气、浮尘、扬沙、沙尘暴天气条件下沙尘粒子谱分布资料。对粒子瞬时谱的统计分析发现:不同的沙尘天气过程中,气溶胶的瞬时浓度存在很大差别。扬沙、沙尘暴天气过程中,气溶胶浓度变化较大;浮尘天气过程中,气溶胶浓度变化较小。沙尘现象越强,粗粒子(d〉2.5μm)越多,各粒径段浓度变化越明显。不同过程,粗细粒子对粒子表面积浓度贡献程度不一。沙尘气溶胶粒子谱型为单峰结构,对粒子的瞬时谱进行了谱型拟合,其具有对数正态分布函数的特征。  相似文献   

2.
敦煌地区春季大气气溶胶粒子数浓度的分析   总被引:6,自引:0,他引:6  
利用2002年春季在敦煌地区戈壁沙漠和绿洲农田观测的大气气溶胶粒子数浓度资料, 分析了它与沙尘天气的关系、谱分布特征以及两种地表下粒子数浓度的差异.结果表明, 不同天气条件下的大气气溶胶粒子数浓度有着不同的特征.在背景天气下, 敦煌地区的大气气溶胶粒子数浓度通常在104L-1以下, 其中以直径在0.5~1.0 μm之间的极细颗粒为主, 绿洲农田细粒子(直径<3.0 μm)的数浓度高于戈壁沙漠, 而较粗粒子(直径>3.0 μm)则相反.当沙尘天气发生时, 该地区的大气气溶胶粒子数浓度增大到105 L-1以上, 直径在1.0~3.0 μm之间的细粒子变为其主要成分, 戈壁沙漠4档的粒子数浓度均高于绿洲农田, 3.0 μm以上的较粗粒子两地的差异更大.  相似文献   

3.
沙暴天气下大气中沙尘粒子空间分布特点及其微结构   总被引:24,自引:0,他引:24       下载免费PDF全文
根据对一次在阿拉善沙漠及其附近地区发生的沙尘暴天气下大气沙尘粒子的飞机观测资料,分析了3600 m以下各层的沙尘含量、粒子谱、云凝结核浓度;讨论了该次沙暴天气下沙尘垂直输送的原因及向下游传输的可能范围和不同距离处的相对沉沙量。  相似文献   

4.
宁夏典型沙尘天气条件下气溶胶分布特征研究   总被引:1,自引:0,他引:1  
利用2006-2010年期间云—大气气溶胶激光雷达红外探索卫星(CALIPSO)星载激光雷达(CALIOP)数据和宁夏地区常规气象观测资料,分析研究了典型沙尘天气条件下宁夏地区大气气溶胶光学性质的分布特征。结果表明:CALIPSO资料能有效地反映宁夏地区沙尘气溶胶相关特性的垂直分布特征。在沙尘天气下,处于贺兰山背风坡海拔较高区域的沙尘可以被抬升到对流层中层以上,近地层大气中主要以粗粒子为主,不规则的非球形气溶胶随着高度的增加而增加,高层大气中以波长比在0.4~2.0之间的粗粒子为主、退偏比在0.4以上的不规则非球形气溶胶在7 km、10 km左右高度出现极大值,这与沙尘天气下湿度垂直分布廓线相一致。在晴空天气条件下,退偏比均在0.2以下,波长比主要在0.2~0.4之间,且两者出现频率随高度的变化较小。在沙尘天气下宁夏地区气溶胶光学厚度主要分布在0.60~2.00之间,晴空天气下主要分布在0.33~0.43之间。  相似文献   

5.
浑善达克沙地沙尘气溶胶的粒谱特征   总被引:22,自引:2,他引:20  
浑善达克沙地是我国主要沙尘气溶胶源地之一,但对其沙尘气溶胶特征一直缺乏研究.2001年4月末到5月初,在内蒙古浑善达克沙地利用PMS Fssp-100型激光粒谱仪进行了大气气溶胶的外场观测,取得了晴天、扬沙和沙尘暴天气条件下沙尘粒子的数浓度采样资料,通过统计分析研究,总结出浑善达克沙地在不同天气条件下近地面沙尘气溶胶的粒谱分布规律.所得统计结果表明了与其他源地沙尘气溶胶的共同点、差异之处及其原因.这一结果也为沙尘气溶胶辐射气候效应的数值模拟提供了新的实测依据.  相似文献   

6.
利用河北省2005年10月份的3次气溶胶飞机观测资料和宏观天气资料,综合分析石家庄地区不同天气条件下气溶胶的垂直分布和尺度谱分布特征。分析结果表明:气溶胶浓度的分布与大气环境情况密切相关。气溶胶数浓度最大值的变化范围是103~104cm-3,平均数浓度为103cm-3,粒子平均直径为0.120~0.150μm;21日近地面有霾,相对湿度为58%,近地面气溶胶浓度较17和29日略低,但粒子平均直径(0.165μm)比其余两次要大,可见相对湿度较大,大气中水汽含量较多,有利于小粒子凝结水汽,使粒子直径增大;逆温层结下,粒子在逆温层下累积,无逆温时数浓度最大值出现在近地面附近。气溶胶粒子谱呈单峰分布。  相似文献   

7.
利用2009年石家庄地区的4次机载PMS探测资料,对不同天气条件下大气气溶胶的数浓度、平均直径垂直分布和谱分布及一次晴天条件下的水平分布进行分析。结果表明:PCASP 探头探测的0.1-3.0 μm气溶胶粒子最大数浓度的量级为102-104 cm-3之间,平均值量级为102-103 cm-3之间,平均直径最大值介于0.225-0.717 μm,平均值介于0.148-0.167 μm。晴天条件下,气溶胶的数浓度随高度递减,直径随高度变化不大;逆温层底气溶胶明显积累,气溶胶浓度在大气边界层内明显高于其他层次;阴天轻雾情况下边界层内的气溶胶数浓度大于雨天和晴天,雨天气溶胶浓度最低;晴天气溶胶数浓度的水平分布不均匀;在云中气溶胶浓度明显下降,在云外气溶胶浓度较高。不同天气条件和晴天不同高度情况下,石家庄地区气溶胶谱型呈单峰分布,小于0.3 μm的细粒子对气溶胶的数浓度贡献最大,且随着高度的增加谱宽变窄。  相似文献   

8.
使用差分淌度粒径分析仪(TDMPS)和空气动力学粒径分析仪(APS)对上甸子区域本底站气溶胶(直径3nm~10μm)数谱分布特征进行观测。利用2008年的观测结果,分析了不同天气(包括沙尘天气、干洁天气和雾霾天气)条件下大气气溶胶数谱分布及其与气象要素和气团来源的关系。结果表明,沙尘天气条件下,上甸子站受西北方向的气团控制,风速较大,粗粒子数浓度明显增加,PM10的质量浓度可以迅速增加到毫克每立方米(mg·m-3)的量级。典型的"香蕉型"新粒子生成事件通常发生在比较干洁晴朗的天气条件下,西北气团主导,大气中背景气溶胶数浓度较低,核模态气溶胶数浓度迅速增长,气溶胶的粒径呈现明显的增长过程,核模态可以平稳地增长到约80nm,达到成为云凝结核的尺度。雾霾天气通常是在西南气团影响下,细颗粒物(1μm以下)不断累积、相对湿度不断升高的条件下发生的。雾霾天气条件下数谱分布的几何中值粒径出现在积聚模态,积聚模态数浓度也高于非雾霾天。个例研究表明,雾霾天气条件下,PM2.5质量浓度可以达到非雾霾天的10倍左右,其中以细颗粒物的贡献为主。在雾霾天气条件下,上甸子站数浓度较高的积聚模态颗粒物主要来自城区的传输,因此对背景地区气溶胶数谱的研究可以为解析城区气溶胶复杂来源提供依据。  相似文献   

9.
利用2009年9月8日华北中南部上空的飞机探测资料,分析了石家庄市和邯郸市区附近大气气溶胶的粒子数浓度、直径、尺度谱分布等时空变化特征。分析表明,降水天气条件下,气溶胶粒子平均数浓度约为137.6个/cm3,平均直径约为0.26μm。气溶胶主要集中于2 000 m以下的对流层低层,气溶胶浓度总体上随高度增加而降低;雨后阴天轻雾天气条件下,气溶胶粒子平均数浓度约为164.7个/cm3,平均直径约为0.16μm。气溶胶在逆温层下累积现象明显,云内气溶胶数浓度明显减少。气溶胶粒子浓度水平变化受下垫面、云区分布等局地因子影响较大。石家庄600 m和6 600 m气溶胶粒子谱呈单峰分布,3 000 m粒子谱呈双峰分布。邯郸6 400 m粒子谱宽较窄,呈单峰分布。  相似文献   

10.
张盼想  张鹏  陈林  王维和  车慧正 《气象科技》2018,46(6):1258-1265
粒子尺度谱和复折射率指数是描述大气气溶胶的基本物理参数,也是遥感大气气溶胶光学厚度的基本假定量,决定了光学厚度遥感的准确程度。本文分析了中国气溶胶遥感网反演的北京周边的沙尘和霾天气下大气气溶胶的体积谱和复折射指数,结果表明:沙尘和霾天气下气溶胶的体积谱均呈现双峰对数正态分布,霾气溶胶粒子体积谱在细模态(0.1~1μm)和粗模态(1~10μm)的占比大体相当,沙尘气溶胶粒子体积谱中粗模态占比远远高于细模态,以粗粒子为主;将实际测量的复折射率同HITRAN 2008数据库中各种类型的气溶胶复折射率光谱数据相比,类沙尘粒子的复折射指数同沙尘气溶胶最为接近,水溶性粒子同霾气溶胶最为接近,在大气气溶胶遥感中如果缺少复折射率的光谱数据,可考虑将类沙尘粒子和水溶性粒子的复折射率光谱数据(0.2~40μm)外推近似代替沙尘和霾气溶胶用于紫外和红外遥感。本研究可为利用紫外光谱和红外光谱定量遥感沙尘和霾气溶胶研究提供参考和依据。  相似文献   

11.
Consideration of sources and growth dynamics of aerosols has led to the conclusion that there may be a distribution or variation of chemical composition and physical structure among atmospheric aerosol particles as a function of size, and within a narrow size range as well. A mathematical representation of these particle properties in terms of an additional dimension to the number size distribution is described. Examples of the relevance of this aspect of aerosol characterization for physical and chemical processes in the atmosphere are discussed. A review of the available techniques shows that several methods are available which can and have provided quantitative results on the distribution of particle properties. Examples of data from the literature have been selected and are presented as three-dimensional distributions illustrating the wide range of particle properties which may exist in narrow size intervals. An evaluation of these results reiterates the value of taking the distribution of particle properties in the atmosphere into account for sampling and modeling purposes.  相似文献   

12.
大气气溶胶尺度分布分形特征研究   总被引:2,自引:0,他引:2       下载免费PDF全文
气溶胶作为大气环境中的重要组成部分,具有复杂的尺度分布结构。为研究其尺度分布特征,采用分形理论首先论述了常用的气溶胶谱分布函数具有分形不变性,然后在分形理论的指导下分别建立了气溶胶粒子和体积分形统计模型,而且以AERONET相关数据验证了分形模型的有效性和实用性,并采用分段分形的方法改进了气溶胶体积分形模型。最后分析研究了分维数的实用意义和分布情况,讨论了气溶胶分维数变化和粒度分布的关系。结果表明:气溶胶粒子数和体积分维数之间存在线性关系,上半年的大气溶胶粒子数分维数的变化幅度明显小于下半年的变化幅度;研究区域大气气溶胶中细粒子分布比较密集,大粒子分布比较分散。分形理论为研究大气气溶胶的尺度分布特征提供了新的方法与手段,具有广阔的研究与应用前景。  相似文献   

13.
In this study the possible conditions for new aerosol particle formation in a background area of Helsinki have been analysed. The measurements of aerosol particle size distribution, main gaseous pollutant compounds, UV spectra and meteorological parameters were performed during April–May 1993. The main interest was concentrated on the investigations of photochemical OH radical formation, the oxidation of gas phase SO2 to H2SO4 and the formation of H2SO4---H2O aerosol particles. The measurements were analysed using a model for OH radical formation and aerosol dynamics. The analysis of aerosol size distributions was carried out using positive matrix factorization. The main conclusion is that based on our model analysis no evidence of new particle formation in the vicinity of the measurement station was found. However, the high concentrations of aerosol particles in the ultrafine size range indicate that some other particle formation pathways are to be considered.  相似文献   

14.
The effects of wintertime and summertime precipitation on the mean (semiannual, seasonal, and monthly) concentration of aerosol particles of different sizes in the atmospheric surface layer are analyzed on the basis of the data of 15-year measurements of atmospheric aerosol in the town of Dolgoprudny (20 km from the center of Moscow). It is demonstrated that a statistically significant negative correlation between the aerosol particle concentration and the precipitation is observed for monthly mean values only and is absent for semiannual and seasonal means. The analysis of individual cases of precipitation corroborated the conclusion on their low impact on the aerosol concentration in the surface layer. In winter, the aerosol concentration decrease is observed within a narrow particle size interval of 0.03?C0.1 ??m and amounts to not more than 30% during several hours. A scavenging effect of summertime precipitation manifests itself in a wider size interval of 0.03?C1.0 ??m but does not exceed 10?C20% and is of short-term nature. The limited effects of precipitation on the surface aerosol are explained by the proximity to the underlying surface being a permanent aerosol source.  相似文献   

15.
A new balloon-borne optical particle counter has been developed to make in situ measurements of stratospheric aerosols. The intensity of light scattered at 60° from the forward direction by individual particles is measured. Aerosol number concentrations in seven size channels can be inferred. The counter has been calibrated using polystyrene and polyvinyl toluene latex spheres. There is good agreement between measured and calculated individual pulse intensities for aerosol with radii from 0.16 to 2.6 µm. The size resolution is limited by broadening of the pulse count/pulse height spectrum, arising mainly from the photoelectron statistics of photomultipliers. Stratospheric aerosol measurements have been made using this instrument at Kiruna (68°N, 21°E), Sweden, in February 1995, and at Aire sur l'Adour (44°N, 0°W), France, in 1992, 1993, and 1994. The uncertainties in the measurements are discussed. The retrieved aerosol concentrations and size distributions are presented, and shown to be broadly consistent with measurements made by the University of Wyoming optical particle counter.  相似文献   

16.
气溶胶光学厚度谱特征判断粒子大小方法初探   总被引:4,自引:0,他引:4       下载免费PDF全文
当气溶胶谱满足Junge分布时,Angstrom指数 (α) 可以准确地描述粒子大小,但真实大气气溶胶很少完全满足这一条件,仅用α判断粒子大小会有较大出入。基于北京、香河、兴隆、太湖4个Aeronet观测站21世纪以来各站历时都超过1年的气溶胶光学厚度资料,获得5511组lnτ与lnλ的二次拟合参数a2,a1,尝试找到一种结合α,a2,a1判断粒子大小的方法。结果表明:当气溶胶为粗粒子时 (Vfine/Vtotal<0.2),α均小于0.75,仅用α就可以较好地判断粒子大小,但当气溶胶以细粒子为主时 (Vfine/Vtotal>0.7),该方法会有较大出入,此时a2,a1可以有效地辅助α判断粒子大小,α>0.75,a2<-0.5或a2<-0.5,a1<-1.0是较好的判据。此外,分析发现国外研究提出的用a2-a1判断粒子大小的方法效果并不理想,尤其在1<a2-a1<2的情况下,粒子的组成有多种可能。  相似文献   

17.
董文 《大气科学》2011,35(5):977-981
气溶胶粒子大小分布是地球环境科学研究中最重要的方向之一.由数学物理模型来估计气溶胶的粒子分布是一个不适定的反问题,反演的目的就是用适定的问题来代替不适定问题,并获得原问题解的近似.本文研究气溶胶粒子分布的约束优化反演方法.首先探讨了问题的病态性,接着基于对待反演参数施加先验约束给出了正则化模型.在正则化的具体实现上,研...  相似文献   

18.
Precipitation scavenging of aerosol particles is an important removal process in the atmosphere that can change aerosol physical and optical properties. This paper analyzes the changes in aerosol physical and optical properties before and after four rain events using in situ observations of mass concentration, number concentration, particle size distribution, scattering and absorption coefficients of aerosols in June and July 2013 at the Xianghe comprehensive atmospheric observation station in China. The results show the effect of rain scavenging is related to the rain intensity and duration, the wind speed and direction. During the rain events, the temporal variation of aerosol number concentration was consistent with the variation in mass concentration, but their size-resolved scavenging ratios were different. After the rain events, the increase in aerosol mass concentration began with an increase in particles with diameter 0.8 μm [measured using an aerodynamic particle sizer(APS)], and fine particles with diameter 0.1 μm [measured using a scanning mobility particle sizer(SMPS)]. Rainfall was most efficient at removing particles with diameter ~0.6 μm and greater than 3.5 μm. The changes in peak values of the particle number distribution(measured using the SMPS) before and after the rain events reflect the strong scavenging effect on particles within the 100–120 nm size range. The variation patterns of aerosol scattering and absorption coefficients before and after the rain events were similar, but their scavenging ratios differed, which may have been related to the aerosol particle size distribution and chemical composition.  相似文献   

19.
Nucleation scavenging and the formation of a cloud interstitial aerosol (CIA) were theoretically studied in terms of the chemical composition of atmospheric aerosol particles. For this study, we used our air-parcel cloud model, which includes the entrainment of air and detailed microphysics, for determining the growth and interaction of aerosol particles and drops. Maritime and remote continental aerosol particle spectrums were used whose size distributions were superpositions of three log-normal distributions, each of a prescribed chemical composition. Our results show (1) that the CIA exhibits a size distribution with a distinctive cut-off at a specific radius of the dry as well as of the wet particle size distribution. All particles above this limiting size become activated to cloud drops and, thus, are not present in the CIA spectrum. This limiting size was found to be independent of the chemical composition of the particles and only dependent on the prevailing supersaturation. Below this specific size, the CIA spectrum becomes depleted of dry aerosol particles in a manner which does depend on their chemical composition and on the supersaturation in the air. (2) The number of aerosol particles nucleated to cloud drops depends critically on the chemical composition of the particles and on the prevailing supersaturation.  相似文献   

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