塔克拉玛干沙漠腹地气溶胶不同波段散射系数比较

利用2010年塔克拉玛干沙漠腹地塔克拉玛干沙漠大气环境观测试验站(下文简称"塔中")多波段(450、525、635 nm)积分浊度计和PM_(10)自动监测仪观测资料,并结合塔中地面气象观测资料,分析了沙漠腹地不同波段气溶胶散射系数的变化特征。分析结果显示:(1)塔中气溶胶对635 nm太阳辐射的散射作用最大,其次是525 nm,最小为450 nm。三波段(450、525、635 nm)散射系数平均值分别为:288.0、318.4、443.8 Mm~(-1)。(2)三波段散射系数日变化与PM_(10)质量浓度一致,都呈单峰变化:夜间高、白天低。在日变化中,散射系数始终保持635 nm最大,525 nm次之,450 nm最小。(3)三波段散射系数年变化基本一致,都与PM_(10)变化接近。1—5月中,除3月散射系数是450 nm最大外,另外4个月均是635 nm最大,450 nm次之,525 nm最小。6—12月散射系数都是635 nm最大,525 nm次之,450 nm最小。(4)三波段散射系数均是沙尘暴下最大,扬沙次之,浮尘最小。不同沙尘天气下,塔中气溶胶对635 nm散射作用都是最明显的,对450 nm和525nm散射作用不同:沙尘暴时,对525 nm的散射强于450 nm,在扬沙和浮尘时,对450 nm的散射强于525 nm,尤其在浮尘时。(5)三波段散射系数与PM_(10)质量浓度都呈显著正相关,PM_(10)质量浓度与525 nm散射系数相关程度最大,450 nm次之,635 nm最小。但是季节内相关程度略有差异:春、冬季PM_(10)浓度与450 nm散射系数相关程度最大,525 nm次之,635 nm最小。夏、秋季则是525nm最大。     

太原冬季大气气溶胶的散射特征

利用积分浊度仪于2005年12月17日-2006年2月14日对太原市区气溶胶散射特性进行了观测分析。结果表明：观测期间气溶胶散射系数小时平均值为（850.2±611.3) Mm-1,散射系数在200～300 Mm-1之间出现的频率最高。太原冬季大气气溶胶散射系数的日变化呈双峰型,散射系数与PM2.5小时平均浓度的线性相关性较好（R2 = 0.82),表明细粒子对散射系数有很大的贡献。观测结果显示气象条件是影响气溶胶散射特性的重要因素之一。     

山西夏季气溶胶散射特征的飞机观测研究

利用3个架次的积分浊度仪和PCASP-100X（Passive Cavity Aerosol Spectrometer Probe）机载观测资料,分析了2013年山西夏季空中有云、无云和少云3种不同条件下气溶胶散射系数的分布特征,讨论了气溶胶散射系数垂直变化与气溶胶数浓度、气象条件的关系,并结合HYSPLIT（Hybrid of Single Particle Lagrangian Integrated Trajectory model）后向轨迹模型研究气溶胶的运动轨迹和可能的污染来源。结果表明:山西夏季空中气溶胶总散射系数变化范围为0～499 Mm-1,晴空气溶胶数浓度和总散射系数明显大于有云和少云时。气溶胶总散射系数一般随高度的增加而递减。造成气溶胶总散射系数、数浓度偏高的原因有下垫面污染源多、风速小、相对湿度高以及逆温层的存在。550 nm波段气溶胶后向散射比大于0.1,粒径0.1～0.5 μm的气溶胶粒子对散射影响最大,说明山西空中细粒子污染比较严重。气溶胶总散射系数与数浓度有一定的相关性。引起气溶胶总散射系数、数浓度较高的气团传输路径主要为西南路径,局地排放的气溶胶大于远距离传输的气溶胶对散射系数的贡献。     

河西春季沙尘气溶胶粒子散射特性的初步研究

利用2008年春季中美沙尘暴联合观测试验中张掖观测站的积分浑浊度仪及同期常规气象资料,分析了有、无沙尘天气下气溶胶总散射系数(550nm)及后向散射比的日变化特征,讨论了一次典型的沙尘暴过程中气溶胶的散射特性。结果表明,在这两种天气状况下,总散射系数日变化都呈双峰型,但峰值大小和出现的时间不同。无沙尘日的气溶胶细粒子所占比例的变化较为明显,日较差比有沙尘日的大。沙尘暴发生时,气溶胶总散射系数有明显的突变,积分浊度仪是对沙尘气溶胶连续监测的有效的工具。     

北京一次污染过程气溶胶光学特性及辐射效应

利用地面激光雷达、太阳光度计观测反演气溶胶光学特性参数,结合PM_2.5观测数据,分析了2018年1月25—28日北京一次完整污染过程中气溶胶光学特性变化。基于观测数据,利用短波辐射传输模式计算了不同程度污染日,晴空背景下气溶胶对辐射加热率的改变程度。结果表明:清洁日（25日）,PM_2.5日平均质量浓度为19.00 μg·m-3,440 nm气溶胶光学厚度为0.13,单次散射反照率为0.87,整层气溶胶消光系数低于0.10 km-1,短波辐射均为增温效应;污染期间（26—27日）,PM_2.5日平均质量浓度为83.21 μg·m-3,气溶胶光学厚度为2.48,气溶胶散射能力增强,单次散射反照率达到0.94,气溶胶主要消光层厚度提升至3.00 km高度,消光系数平均值为0.43 km-1,气溶胶在垂直方向的变化导致气溶胶中上层（1.50~3.00 km高度）加热作用强烈,短波辐射加热率平均值达到13.89 K·d-1,而低层（1.50 km高度以内）加热作用较弱,加热率平均值仅为0.99 K·d-1。气溶胶散射能力增强导致加热作用减弱,污染日加热率对于气溶胶散射能力变化更敏感。     

半干旱地区气溶胶散射和吸收特性的观测研究

利用兰州大学半干旱气候和环境观测站SACOL（Semi-Arid Climate and Environment Observatory of Lanzhou University）2007年11月1日-2008年10月31日AE-31黑碳仪和2007年8月1日-2008年7月31日M9003积分浊度仪的连续观测资料,对该地区气溶胶散射和吸收特性的变化特征进行了分析。结果表明,该地区气溶胶年平均散射系数为158.86M.m-1,吸收系数为14.11M.m-1,520nm单次散射比为0.83;散射系数和吸收系数的年变化呈单峰型,峰值分别出现在12月和11月;采暖期内日变化呈双峰型,非采暖期内近似表现为单峰型。在沙尘天气条件下,散射系数和吸收系数分别增大了103.8%和88.5%。结合同期APS-3321粒子谱仪的相关观测资料分析得出,无论是粒子数浓度还是质量浓度,与散射系数和吸收系数的相关系数均在0.8以上。     

南京北郊气溶胶粒子的光学散射特征

利用三波段积分浊度仪对南京北郊2009-2010年四季气溶胶散射系数进行观测和分析。结果表明：气溶胶散射系数具有明显的季节变化特征,春季最低,秋季最高,冬夏季差别不大;气溶胶散射系数变化范围为51．6～2748．3Mm-1,平均值为478．6Mm-1。气溶胶散射系数的日变化特征为双峰型。空气相对湿度与气溶胶散射系数呈正相关关系：地面风向与气溶胶散射系数关系密切,偏东风时气溶胶散射系数最大,偏南风和偏西风时气溶胶散射系数较小。降水对气溶胶有明显的清除作用。能见度大于5km时,能见度与散射系数呈负相关关系。四季大气中SO2和NO2与气溶胶散射系数存在一定相关性,其中秋季SO,与气溶胶散射系数的相关系数最大（0．68）,春季NO2与散射系数的相关系数最大（0．62）,均通过0．05信度的显著性检验。     

利用FY-4A卫星光学数据对中国近地面PM2.5浓度的估算和检验分析

对FY-4A卫星的气溶胶光学厚度（AOD）产品进行检验,并根据卫星相关观测资料,通过改进后的PMRS方法,反演得到中国近地面PM_2.5质量浓度网格化分布。结果表明,FY-4A卫星反演不同站点AOD与地基观测网（AERONET）观测结果吻合较好,但存在一定的低估或高估现象,相关系数区间为0.54—0.87。将细粒子比（FMF）以0.4为界进行划分,FMF＞0.4时,拟合结果较FMF≤0.4时更接近于AERONET观测结果;但FMF≤0.4时,卫星反演的AOD稳定性优于FMF＞0.4时。通过引入AOD的大小,改进FMF＞0.4时对细粒子柱状体积消光比（VE_f）的估算算法,并通过改进后的PMRS方法对中国近地面PM_2.5浓度进行逐时反演,其反演结果和地面观测结果相关较好,其中,乌鲁木齐、石家庄和徐州观测点的相关系数均高于0.7,但数值上仍存在高估或低估,误差结果由多种因素决定。空间分布中,卫星反演的中国2019年近地面PM_2.5浓度月均值与近地面观测的结果有较好的对应关系,二者逐月演变趋势基本一致,基本可以反映出中国近地面大气细粒子的空间分布,特别是秋、冬季京津冀周边区域、汾渭平原等污染高值区均与地面观测对应较好。      

2010年长江三角洲临安本底站PM2.5理化特征

2010年在代表长三角区域背景地区的浙江省临安区域大气本底站开展了对大气细粒子PM_2.5为期1年的地面观测,并对细粒子中水溶性离子和碳组分的季节变化特征进行了分析。临安2010年大气中PM_2.5质量浓度平均为 (58.2±50.8) μg·m－3,PM_2.5质量浓度季节变化明显。利用HYSPLIT4模式计算了2010年临安72 h后向轨迹,根据轨迹计算与聚类结果,结合地面观测的PM_2.5数据进行了分析。研究表明:临安地区因受到长江三角洲区域及偏北气流引起的污染传输影响,呈现出高细粒子水平特征。PM_2.5中总水溶性离子年平均质量浓度为 (28.5±17.7) μg·m－3,占PM_2.5质量浓度的47%。其中,气溶胶组分SO₄2-,NO₃-和NH₄+所占比例最大,共占总水溶性离子的69%。PM_2.5中有机碳和元素碳的年平均质量浓度分别为 (10.1±6.7) μg·m－3和 (2.4±1.8) μg·m－3。有机碳和元素碳质量浓度显著相关,表明有机碳和元素碳主要来自相同的排放源。     

一种改进的TSI3563积分浊度误差校正方法

TSI3563型积分式浊度计是一种性能出色的气溶胶散射系数观测仪器,然而由于仪器设计所固有的限制,TSI3563型浊度计观测结果包含有角度截断和非朗伯体光源两项系统性误差,会使观测结果较真值偏小10%左右。因此,需要对TSI3563型浊度计的观测结果进行校正才能得到较为精确的散射系数观测值。该研究利用2009年华北平原HaChi气溶胶外场观测数据测试了现有校正方法,结果显示,传统的校正方法在我国华北平原这样的高气溶胶污染地区并不适用。为此,提出一种改进的校正方法,利用同时观测的PM₁和PM₁₀数据,在校正方案中加入超微米粒子体积比这一参量,对于不同体积比采用不同的校正函数。利用实际观测数据检验后发现,改进方法的校正效果相对于传统方法有很大改善。     

中国大气气溶胶辐射特性参数的观测与研究进展

长期系统的气溶胶辐射特性观测资料是定量研究气溶胶辐射和气候效应的重要基础.本文综合介绍中国大气气溶胶辐射特性观测与研究现状和成果,重点包括以下内容:地面太阳光度计联网观测气溶胶光学厚度、单次散射反照率、尺度谱;从全波段太阳辐射反演气溶胶光学厚度、单次散射反照率;浊度计和黑碳仪测量地面气溶胶散射系数和吸收系数;地基/星载激光雷达观测气溶胶(后向散射系数)垂直分布;极轨/静止卫星遥感反演气溶胶光学特性.     

The impacts of optical properties on radiative forcing due to dust aerosol

There are large uncertainties in the quantitative assessment of radiative effects due to atmospheric dust aerosol. The optical properties contribute much to those uncertainties. The authors perform several sensitivity experiments to estimate the impacts of optical characteristics on regional radiative forcing in this paper. The experiments involve in refractive indices, single scattering aibedo, asymmetry factor and optical depth. An updated dataset of refractive indices representing East Asian dust and the one recommended by the World Meteorology Organization （WMO） are contrastively analyzed and used. A radiative transfer code for solar and thermal infrared radiation with detailed aerosol parameterization is employed. The strongest emphasis is on the refractive indices since other optical parameters strongly depend on it, and the authors found a strong sensitivity of radiative forcing on refractive indices. Studies show stronger scattering, weaker absorption and forward scattering of the East Asian dust particles at solar wavelengths, which leads to higher negative forcing, lower positive forcing and bigger net forcing at the top of the atmosphere （TOA） than that of the WMO dust model. It is also found that the TOA forcings resulting from these two dust models have opposite signs in certain regions, which implies the importance of accurate measurements of optical properties in the quantitative estimation of radiative forcing.     

Aerosol Hygroscopicity during the Haze Red-Alert Period in December 2016 at a Rural Site of the North China Plain

A humidification system was deployed to measure aerosol hygroscopicity at a rural site of the North China Plain during the haze red-alert period 17–22 December 2016. The aerosol scattering coefficients under dry [relative humidity (RH) < 30%] and wet (RH in the range of 40%–85%) conditions were simultaneously measured at wavelengths of 450, 550, and 700 nm. It is found that the aerosol scattering coefficient and backscattering coefficient increased by only 29% and 10%, respectively when RH went up from 40% to 80%, while the hemispheric backscatter fraction went down by 14%, implying that the aerosol hygroscopicity represented by the aerosol scattering enhancement factor f(RH) is relatively low and RH exerted little effects on the aerosol light scattering in this case. The scattering enhancement factors do not show significant differences at the three wavelengths, only with an approximate 2% variation, suggesting that the aerosol hygroscopicity is independent of the wavelength. Aerosol hygroscopicity is highly dependent on the aerosol chemical composition. When there is a large mass fraction of inorganics and a small mass fraction of organic matter, f(RH) reaches a high value. The fraction of NO₃^– was strongly correlated with the aerosol scattering coefficient at RH = 80%, which suggests that NO₃^– played an important role in aerosol hygroscopic growth during the heavy pollution period.     

Airborne and lidar measurements of aerosol and cloud particles in the troposphere over Alert Canada in April 1986

As a component of the Canadian Arctic Haze Study, held coincident with the second Arctic Gas and Aerosol Sampling Program (AGASP II), vertical profiles of aerosol size distribution (0.17 m), light scattering parameters and cloud particle concentrations were obtained with an instrumented aircraft and ground-based lidar system during April 1986 at Alert. Northwest Territories. Average aerosol number concentrations range from about 200 cm^–3 over the Arctic ice cap to about 100 cm^–3 at 6 km. The aerosol size spectrum is virtually free of giant or coarse aerosol particles, and does not vary significantly with altitude. Most of the aerosol volume is concentrated in the 0.17–0.50 m size range, and the aerosol number concentration is found to be a good surrogate for the SO₄ ⁼ concentration of the Arctic haze aerosol. Comparison of the aircraft and lidar data show that, when iced crystal scattering is excluded, the aerosol light scattering coefficient and the lidar backscattering coefficient are proportional to the Arctic haze aerosol concentration. Ratios of scattering to backscattering, scattering to aerosol number concentration, and backscattering to aerosol number concentration are 15.3 steradians, 1.1×10^–13 m², and 4.8×10^–15 m² sr^–1, respectively. Aerosol scattering coefficients calculated from the measured size distributions using Mie scattering agree well with measured values. The calculations indicate the aerosol absorption optical depth over 6 km to range between 0.011 and 0.018. The presence of small numbers of ice crystals (10–20 crystals 1^–1 measured) increased light scattering by over a factor of ten.     

西北地区气溶胶光学特性及辐射影响

利用SACOL（兰州大学半干旱气候与环境观测站）2006~2012年AERONET（全球气溶胶自动监测网）level 2.0和太阳短波辐射计资料,分析了中国西北地区气溶胶的光学特性与辐射影响。利用辐射传输模式SBDART（平面平行大气辐射传输模式）检验TOA（大气层顶）处辐射强迫为正的原因。BOA（地表）、TOA、Atmosphere（大气）的辐射强迫年均值分别是-59.43 W m-2、-17.03 W m-2、42.40 W m-2,AOD（光学厚度,550 nm）年均值0.37,α（波段的波长指数,440~675 nm）年均值0.91,变化趋势与AOD位相相反,当AOD为0.3~2.2时,α很小（0.0~0.2）,表明粒子尺度很大。SSA（单次散射反照率,675 nm）年均值0.93,g（不对称因子,675 nm）年均值0.68,复折射指数（675 nm）实部年均值1.48,虚部0.007。复折射指数实部的年变化趋势与AOD一致,虚部与AOD反位相,所以西北地区多为粗模态散射性气溶胶。气溶胶对大气的加热率最大值出现在0~2 km,随高度递减。冬、夏半年在地表加热率分别是2.6 K d-1和0.6 K d-1;季节变化中,冬季、秋季、春季和夏季,在地表的加热率依次是2.5 K d-1、1.4 K d-1、1.2 K d-1和0.2 K d-1,主要因为秋季气溶胶的吸收性大于春季。地表反照率和SSA对TOA正辐射强迫贡献率分别是22.5%和77.5%。     

A study of aerosol properties over Lahore (Pakistan) by using AERONET data

It is well established that aerosols affect the climate in a variety of ways. In order to understand these effects, we require an insight into the properties of aerosols. In this paper we present a study of aerosol properties such as aerosol optical depth (AOD), single scattering albedo (SSA) and aerosol radiative forcing (ARF) over mega city of Lahore (Pakistan). The data from Aerosol Robotic Network (AERONET) have been used for the period December 2009 to October 2011. The seasonal average values of AOD, asymmetry parameter (ASY) and volume size distribution in coarse mode were observed to be highest in summer. On the other hand, the average values of Angstrom exponent (AE) and imaginary part of refractive index (RI) were found to be maximum in winter. The average value of real part of RI was found to be higher in spring than in all other seasons. The SSA exhibited an increasing trend with wavelength in the range 440 nm–1020 nm in spring, summer and fall indicating the dominance of coarse particles (usually dust). However, a decreasing trend was found in winter in the range 675 nm–1020 nm pointing towards the dominance of biomass and urban/industrial aerosols. As far as aerosol radiative forcing (ARF) is concerned, we have found that during the spring season ARF was lowest at the surface of Earth and highest at top of the atmosphere (TOA). This indicates that the atmosphere was warmer in spring than in all the remaining seasons.     

Aerosol polarized phase function and single-scattering albedo retrieved from ground-based measurements

Aerosol optical parameters, polarized phase function and single-scattering albdeo, have been retrieved from ground-based sun photometer measurements in Beijing 2003. The measured aerosol optical thickness varies from 0.12 to 0.77 with an average value of 0.39. The measured Ångström coefficient ranges from 0.75 to 1.47 with an average value of 1.21. The retrieved single-scattering albedo at 870 nm is within the 0.76–0.94 range and the average value is 0.85, suggests there are considerable aerosol absorptions in Beijing. The maximum value of retrieved polarized phase function at 870 nm ranges from 0.068 to 0.225 with an average value of 0.16, and it illustrates good correlations with the Ångström coefficient, i.e. the relative size of aerosol particles. Analyses of measurements and theoretical calculations show the polarized phase function is sensitive to aerosol size distribution and complex refractive index, especially the imaginary part of the refractive index which denotes aerosol light absorbing effects. These results suggest that the polarized phase function is an effective and unique aerosol optical parameter and is able to improve the retrieval of aerosol physical properties.     

THE IMPACT OF RELATIVE HUMIDITY ON THE RADIATIVE PROPERTY AND RADIATIVE FORCING OF SULFATE AEROSOL*

With the data of complex refractive index of sulfate aerosol,the radiative properties of the aerosol under 8 relative humidity conditions are calculated in this paper.By using the concentration distribution from two CTM models and LASG GOALS/AGCM,the radiative forcing due to hygroscopic sulfate aerosol is simulated.The results show that:(1)With the increase of relative humidity,the mass extinction coefficiency factor decreases in the shortwave spectrum;single scattering albedo keeps unchanged except for a little increase in longwave spectrum,and asymmetry factor increases in whole spectrum.(2)Larger differences occur in radiative forcingsimulated by using two CTM data,and the global mean forcing is -0.268 and -0.816 W/m²,respectively.(3)When the impact of relative humidity on radiative property is taken into account,the distribution pattern of radiative forcing due to the wet particles is very similar to that of dry sulfate,but the forcing value decreases by 60%.