齐次积分方程数值求解法及在反演气溶胶谱分布上的应用

本文论述了一个数值求解齐次的第一类Fredholm积分方程的方法,并以消光系数和体积散射系数综合反演气溶胶谱分布为例,说明采用比值通道以反演气溶胶谱分布有利于消除多次散射等系统误差.本文还证明了在Junge谱分布下,不同波长的体积消光系数、散射相函数等Mie散射光学参数之比与折射率无关的特性,指出了采用比值通道能够有效地消除折射率的不确定性对于消光——小角散射法反演气溶胶谱分布的影响.     

湿气溶胶的光散射特性

在不同干气溶胶谱分布以及激光波长为6943埃的条件下,根据三种湿气溶胶模式,理论计算了湿气溶胶的消光系数和体后向散射微分截面,并分析讨论了它们随相对湿度的变化规律。     

大气气溶胶对激光的消光的理论计算

计算了某几类大气气溶胶谱分布对0.6943μ、 1.06μ和10.6μ等几个波长的消光特性。结果表明利用能见度确定激光大气消光系数的可能和局限。     

2007年冬季大连市区气溶胶垂直剖面特征

选用2007年1月8—30日期间8个无云天的激光雷达资料进行分析。基于Fernald方法反演得到气溶胶消光系数廓线,结合无线电探空资料分析了边界层内气溶胶时空分布,并将反演的激光雷达最低观测高度处(180 m)的气溶胶消光系数与地面PM10、能见度资料进行对比分析。结果表明：冬季大连市区气溶胶主要分布在2 km以下区域,早晨和夜间在0.5 km以下区域经常存在一个气溶胶层;气溶胶消光系数廓线与探空资料较吻合;反演激光雷达最低观测高度处(180 m)的气溶胶消光系数与地面的PM10浓度呈正相关,与能见度呈负相关,相关性较好。     

沈阳地区大气气溶胶消光特性的观测研究

利用沈阳地区2010年全年大气总消光系数、气体分子吸收系数、气溶胶吸收和散射系数以及大气可吸入颗粒物数浓度的小时数据,对沈阳地区的大气消光特别是气溶胶消光性质进行了高时间分辨率的研究。结果表明:总消光系数和气溶胶散射系数在一天内呈单周期峰谷型分布,05—06时(北京时间,下同)达到峰值,15时达到谷值。大气总消光系数在雪天最大、霾天次之、晴天最小。气溶胶消光系数与粒子数浓度的相关性随着粒径的减小而增大。     

济南市一次晴空气溶胶粒子的特征分析

利用１９８９年１０月１７日在济南上空进行晴空探测所获得的ＰＭＳ资料及０８时济南气象观测资料，对济南市上空大气气溶胶粒子的浓度分布、谱分布及消光系数等微物理特性作了比较详细的分析。并初步探讨了一些气象因子与气溶胶粒子浓度分布的关系。     

成都一次重污染过程的气溶胶光学特性垂直分布

利用微脉冲激光雷达观测数据、PM_(2.5)浓度数据、地面气象观测资料和探空数据对成都2017年1月1—6日连续出现的重污染过程进行分析研究。结果表明:激光雷达反演的消光系数演变与PM_(2.5)浓度值变化对应一致,PM_(2.5)浓度升高,近地面消光系数增大;反之,则近地面消光系数减小。对于此次过程,在无冷空气影响时,混合层高度和相对湿度的日变化对消光系数廓线有明显影响,混合层高度降低,大气环境容量减小,相对湿度增加,气溶胶吸湿增长,消光系数增大,地面污染加重。天空状况对气溶胶垂直分布影响显著,晴天或多云天气,早晨强逆温使得水汽和大量气溶胶集中在逆温层顶以下区域,地面污染严重;中午混合层发展,使得混合层内的气溶胶均匀混合,气溶胶层变厚,近地面消光系数显著减小,地面污染减轻。在前一日为晴天或多云天气,当天为阴天时,早上气溶胶明显分为两层,一层在近地面,另一层在残留层顶附近;中午由于垂直湍流增强,一部分残留层气溶胶向下混合至混合层内,使得混合层内的气溶胶粒子增多,地面污染加重,消光系数明显增加。近地面强逆温层、混合层高度降低、残留层气溶胶向下混合、相对湿度增加均是导致地面污染加重的原因。     

成都夏季气溶胶消光特性研究

本文利用成都2017年6~8月的米散射微脉冲激光雷达观测数据,对成都夏季气溶胶消光系数、边界层高度以及气溶胶光学厚度进行了反演,并结合太阳光度计观测资料、地面颗粒物浓度以及大气能见度数据研究了气溶胶消光系数日变化与月变化规律,气溶胶消光系数的垂直分布特征及影响因素。结果表明:气溶胶消光系数的日变化受人类活动以及边界层日变化影响显著,表现出凌晨与傍晚最大,早晨次之,午后最小的特征。消光高值出现在200m以下和300~700m的高度区间,夜间观察到的消光高值可能与颗粒物在夜间近地面浓度较高以及本地夜间降水频发有关。激光雷达反演的消光系数与光度计反演的气溶胶光学厚度在夏季各月的表现一致,夏季各月消光极值均出现在100~150m的近地面层。近地面消光系数与地面颗粒物浓度之间具有较好的正相关,并且粒子粒径更小时相关性更好。气溶胶光学厚度主要来自低层大气的贡献,0.1~0.2μm的细粒子气溶胶占比对于大气消光有主要影响,但气溶胶对大气的消光影响除了与粒子浓度有关,还与粒子的理化性质有关。      

基于微脉冲激光雷达观测资料的半干旱区沙尘天气消光效应分析

利用兰州大学半干旱区气候与环境观测站（SOCAL）的微脉冲激光雷达（MPL）2008年4月30日至5月2日观测资料,对晴朗天气、浮沉天气及扬沙天气过程中气溶胶垂直分布的连续变化、物理机制进行了对比分析与探讨。结果表明MPL很好地反映出不同天气过程中大气气溶胶廓线的日变化特征：受人类活动影响,天气晴朗时,早晨9时开始在0—2km范围出现气溶胶聚集区,持续至15时,气溶胶平均消光系数〈0．20km-1;受沙尘输送影响,浮尘天气时,气溶胶聚集区高度范围为1—2km,高层气溶胶富集区高度范围为5—7km,气溶胶平均消光系数0．38km-1;扬沙天气时,气溶胶聚集区高度范围为0—1km,浓度远大于浮尘天气,但高层气溶胶浓度较小且分布较均匀,气溶胶平均消光系数〉0．50km-1。     

利用MODIS卫星和激光雷达遥感资料研究香港地区的一次大气气溶胶污染

利用MODIS可见光通道气溶胶光学厚度的卫星遥感和523 nm波长微脉冲激光雷达 (MPL LIDAR) 对气溶胶消光系数垂直分布的观测，分析了珠江三角洲地区2003年6月一次气溶胶污染过程中气溶胶光学厚度的分布特征、气溶胶消光系数廓线的演变，认为这次污染过程是弱高压控制下的区域性污染，而香港地区污染物浓度的上升与区域性输送有直接关系，结果表明卫星和激光雷达的光学遥感方法提供了研究大气污染的可行手段。     

DISTRIBUTION OF AEROSOL EXTINCTION IN THE LOWER TROPOSPHERE BY MICRO-PULSE LIDAR OBSERVATION

The profiles of aerosol extinction coefficients are investigated by micro-pulse lidar(MPL)combined with the meteorological data in the lower troposphere at Meteorological ResearchInstitute(MRI).Japan.Larger extinction values of aerosol are demonstrated in the nocturnalstable air layer with larger Richardson number,and light wind velocities are favorable for aerosolconcentrating in the planetary boundary layer(PBL).But aerosol extinction coefficients showlarger values over the altitudes of 2.0 to 5.0km where correspond to higher relative humidity(RH).The tops of PBL identified by the aerosol extinction profiles almost agree with ones byradiosonde data.The diurnal variations of aerosol extinction profiles are clearly displayed,intensive aerosol layers usually are formed over the period of mid-morning to 1400 Loeal Time(LT).then elapse in the cloudless late afternoon and nighttime.Thermal eonvection or turbulenttransport from the surfaee probably dominates these temporal and spatial changes of aerosoldistribution.     

DISTRIBUTION OF AEROSOL EXTINCTION IN THE LOWER TROPOSPHERE BY MICRO-PULSE LIDAR OBSERVATION*

The profiles of aerosol extinction coefficients are investigated by micro-pulse lidar(MPL) combined with the meteorological data in the lower troposphere at Meteorological Research Institute(MRI).Japan.Larger extinction values of aerosol are demonstrated in the nocturnal stable air layer with larger Richardson number,and light wind velocities are favorable for aerosol concentrating in the planetary boundary layer(PBL).But aerosol extinction coefficients show larger values over the altitudes of 2.0 to 5.0km where correspond to higher relative humidity(RH).The tops of PBL identified by the aerosol extinction profiles almost agree with ones by radiosonde data.The diurnal variations of aerosol extinction profiles are clearly displayed,intensive aerosol layers usually are formed over the period of mid-morning to 1400 Loeal Time(LT).then elapse in the cloudless late afternoon and nighttime.Thermal eonvection or turbulent transport from the surfaee probably dominates these temporal and spatial changes of aerosol distribution.     

宽带消光法反演气溶胶光学厚度与AERONET北京站探测结果的对比研究

该文简要介绍了遥感气溶胶光学厚度的宽带消光法, 重点比较与分析了2001～2002年间北京地区宽带消光法和全球气溶胶探测网(AERONET)气溶胶光学厚度的探测结果.对比结果表明, 两类探测结果在无云晴天的条件下具有很好的吻合, 二者的相关系数达到90%以上.另外, 作者还针对宽带消光法反演月平均气溶胶光学厚度问题, 提出了一个减小云对反演结果影响的方法, 即月平均光学厚度约束法, 并与全球气溶胶探测网探测结果做对比分析.二者结果的一致性表明该约束方法的有效性.     

An Empirical Method for Estimating Background Stratospheric Aerosol Extinction Profiles over China

The current paper introduces an empirical method for estimating the vertical distribution of background stratospheric aerosol extinction profiles covering the latitude bands of 50±5°N,40±5°N,30±5°N,and 20±5°N and the longitude range of 75 135°E based on Stratospheric Aerosol and Gas Experiment (SAGE) II aerosol extinction measurements at wavelengths of 1020 nm,525 nm,452 nm,and 386 nm for the volcanically calm years between 1998 2004.With this method,the vertical distribution of stratospheric aerosol extinction coefficients can be estimated according to latitude and wavelength.Comparisons of the empirically calculated aerosol extinction profiles and the SAGE II aerosol measurements show that the empirically calculated aerosol extinction coefficients are consistent with SAGE II values,with relative differences within 10% from 2 km above the tropopause to 33 km,and within 22% from 33 km to 35 km.The empirically calculated aerosol stratospheric optical depths (vertically integrated aerosol extinction coefficient) at the four wavelengths are also consistent with the corresponding SAGE II optical depth measurements,with differences within 2.2% in the altitude range from 2 km above the tropopause to 35 km.     

Vertical distributions of aerosol optical properties during haze and floating dust weather in Shanghai

A comparative study on the vertical distributions of aerosol optical properties during haze and floating dust weather in Shanghai was conducted based on the data obtained from a micro pulse lidar.There was a distinct difference in layer thickness and extinction coefficient under the two types of weather conditions.Aerosols were concentrated below 1 km and the aerosol extinction coefficients ranged from 0.25 to 1.50km^-1 on haze days.In contrast,aerosols with smaller extinction coefficients(0.20 0.35 km^-1) accumulated mainly from the surface to 2 km on floating dust days.The seasonal variations of extinction and aerosol optical depth（AOD） for both haze and floating dust cases were similar greatest in winter,smaller in spring,and smallest in autumn.More than 85%of the aerosols appeared in the atmosphere below 1 km during severe haze and floating dust weather.The diurnal variation of the extinction coefficient of haze exhibited a bimodal shape with two peaks in the morning or at noon,and at nightfall,respectively.The aerosol extinction coefficient gradually increased throughout the day during floating dust weather.Case studies showed that haze aerosols were generated from the surface and then lifted up,but floating dust aerosols were transported vertically from higher altitude to the surface.The AOD during floating dust weather was higher than that during haze.The boundary layer was more stable during haze than during floating dust weather.     

Aerosol climatology for the planetary boundary layer derived from regular lidar measurements

Regular aerosol extinction and backscatter measurements using a UV Raman Lidar have been performed for almost 3 years in Hamburg in the frame of the German Lidar Network. A set of 92 aerosol extinction and 164 aerosol backscatter profiles has been used for statistical investigations. Mean values and variances of the aerosol extinction and backscatter in the boundary layer have been calculated. Large fluctuations during the whole year have been found. The measured aerosol extinction over Hamburg shows a seasonal cycle with highest values in early fall and a second less prominent peak in spring.An analysis of the data using back trajectories showed a dependence of the aerosol extinction on the origin of the air mass. The residence time of the air mass over industrialized areas was found to be an important parameter for the measured aerosol extinction at Hamburg. However, only a small part of the total variability could be explained by the air mass origin.For 75 cases of aerosol extinction measurements under cloud-free conditions, the aerosol backscatter profile and therefore, the lidar ratio as a function of altitude could be determined. Winter measurements of the lidar ratio are often close to model results for maritime aerosol, the summer measurements are close to the model results for urban or continental aerosols.The high quality of the data has been proven by intercomparisons with other lidar systems and with star photometer measurements of the aerosol optical depth during the Lindenberg Aerosol Characterization Experiment (LACE'98) field campaign.     

A Closure Study of Aerosol Hygroscopic Growth Factor during the 2006 Pearl River Delta Campaign

Measurements of aerosol physical, chemical and optical parameters were carried out in Guangzhou, China from 1 July to 31 July 2006 during the Pearl River Delta Campaign. The dry aerosol scattering coefficient was measured using an integrating nephelometer and the aerosol scattering coefficient for wet conditions was determined by subtracting the sum of the aerosol absorption coefficient, gas scattering coefficient and gas absorption coefficient from the atmospheric extinction coefficient. Following this, the aerosol hygroscopic growth factor, f(RH), was calculated as the ratio of wet and dry aerosol scattering coefficients. Measurements of size-resolved chemical composition, relative humidity (RH), and published functional relationships between particle chemical composition and water uptake were likewise used to find the aerosol scattering coefficients in wet and dry conditions using Mie theory for internally- or externally-mixed particle species [(NH₄)₂SO₄, NH₄NO₃, NaCl, POM, EC and residue]. Closure was obtained by comparing the measured f(RH) values from the nephelometer and other in situ optical instruments with those computed from chemical composition and thermodynamics. Results show that the model can represent the observed f(RH) and is appropriate for use as a component in other higher-order models.     

气溶胶辐射效应在华东地区一次雾霾过程中的作用

利用WRF/Chem(Weather Research and Forecasting Model coupled with Chemistry)模拟了2013年12月华东地区一次雾、霾事件气溶胶辐射反馈效应对气象场和大气质量的影响。通过3个不同气溶胶浓度设置的试验区分气溶胶浓度不同辐射效应的影响。比较不同试验得出,本次雾、霾过程中,不论是气溶胶直接、半直接辐射效应还是间接效应均使污染地区短波辐射减少、2 m气温下降、大气边界层高度降低,不利于水汽与污染物的扩散,空气污染进一步加重,雾结构进一步稳定,并使雾的持续时间延长,发展高度更高;对于化学场来说,气溶胶直接、半直接辐射效应使污染地区PM_(2.5)浓度增大、消光系数增大、氮氧化物浓度增大,臭氧浓度降低;间接辐射效应使PM_(2.5)浓度和消光系数进一步增大,氮氧化物、臭氧浓度降低。综上所述,气溶胶辐射效应能使大气污染加重,并利于雾的发生、发展。     

Retrieval of the single scattering albedo of Asian dust mixed with pollutants using lidar observations

The vertical distribution of single scattering albedos （SSAs） of Asian dust mixed with pollutants was derived using the multi-wavelength Raman lidar observation system at Gwangju （35.10°N,126.53°E）.Vertical profiles of both backscatter and extinction coefficients for dust and non-dust aerosols were extracted from a mixed Asian dust plume using the depolarization ratio from lidar observations.Vertical profiles of backscatter and extinction coefficients of non-dust particles were input into an inversion algorithm to retrieve the SSAs of non-dust aerosols.Atmospheric aerosol layers at different heights had different light-absorbing characteristics.The SSAs of non-dust particles at each height varied with aerosol type,which was either urban/industrial pollutants from China transported over long distances at high altitude,or regional/local pollutants from the Korean peninsula.Taking advantage of independent profiles of SSAs of non-dust particles,vertical profiles of SSAs of Asian dust mixed with pollutants were estimated for the first time,with a new approach suggested in this study using an empirical determination of the SSA of pure dust.The SSAs of the Asian dust-pollutants mixture within the planetary boundary layer （PBL） were in the range 0.88-0.91,while the values above the PBL were in the range 0.76-0.87,with a very low mean value of 0.76 ± 0.05.The total mixed dust plume SSAs in each aerosol layer were integrated over height for comparison with results from the Aerosol Robotics Network （AERONET） measurements.Values of SSA retrieved from lidar observations of 0.92 ± 0.01 were in good agreement with the results from AERONET measurements.