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1.
In this paper the effects of aerosol on tropospheric ozone measurements by three-wavelength (266-289-308nm) dual differential absorption lidar (DIAL) and two-wavelength (266-289 nm and 266-308 nm) DIAL are simulated.By using the two kinds of DIAL.vertical profiles of ozone density from 2 to 3.6 km altitude range are measured.Both simulation and observation results show that the three-wavelength dual-DIAL method is more effective to reduce the effects of aerosol than the two-wavelength DIAL method.Therefore,accurate ozone density distributions can be retrieved by the three wavelength dual DIAL method.  相似文献   

2.
双差分激光雷达——一组可以提高臭氧测量精度的波长   总被引:1,自引:0,他引:1  
模拟了气溶胶影响三波长双差分 (2 6 6 - 2 89- 30 8nm)方法和双波长差分 (2 6 6 - 2 89nm和 2 6 6 - 30 8nm)方法测量对流层臭氧的误差 ,并在合肥测量了对流层 2~ 3.6km高度的臭氧分布。结果表明 ,三波长双差分方法比常规的双波长差分方法能更有效地克服气溶胶的影响 ,三波长差分测量的结果比常规的双波长差分的结果更精确。同时还揭示了气溶胶影响双波长差分方法测量臭氧的规律。模拟结论与测量结果是一致的  相似文献   

3.
王志恩  胡欢  陵周军 《气象学报》1996,54(4):437-446
文中提出了一种新的激光雷达测量臭氧的方法:双差分吸收方法。理论分析和数值模拟表明这种方法可以有效减小气溶胶消光和后向散射对臭氧测量的影响,从而使激光雷达在气溶胶影响严重地区测量的臭氧精度比传统差分吸收激光雷达大大提高。利用(289,313;277.1,299.1nm)或(268.4,289;277.1,299.1nm)4波长进行双差分吸收可以用于对流层大气气溶胶含量丰富或分布不均匀地区臭氧的测量。利用(299.1,341.5;308,353nm)4波长进行双差分吸收可以对火山爆发后平流层臭氧进行较精确的测量。  相似文献   

4.
利用2014年夏季在河北饶阳开展的“华北区域光化学立体试验”观测得到气溶胶辐射特性,根据三波长角散射浊度仪Aurora 4000测量获取的前向角散射系数(10°~90°)和后向散射系数,提出了一种基于浊度仪直接测量的气溶胶角散射系数和改进的HG相函数近似获取气溶胶散射相函数、不对称因子的拟合估算方法。分析了2014年6月16日—8月18日夏季观测试验期间河北饶阳地区大气气溶胶细粒子(PM2.5)在635 nm,525 nm,450 nm 3个波段的不对称因子、相函数等的变化特征。结果表明:用改进的HG相函数近似能够较好地拟合河北饶阳实际观测的PM2.5的气溶胶散射相函数。拟合得到河北饶阳地区观测期间干气溶胶细粒子在3个波段的平均不对称因子(g)分别为0.53±0.04(635 nm),0.57±0.05(525 nm)和0.57±0.07(450 nm)。  相似文献   

5.
青藏高原上空气溶胶含量的分布特征及其与臭氧的关系   总被引:7,自引:5,他引:2  
采用1991年10月—2005年11月的HALOE资料,分析了青藏高原(27°~40°N,75°~105°E)上空气溶胶数密度、体积密度、面积密度的分布和变化特征,探讨了它们与臭氧的关系,并且与同纬度带中国东部地区(107°~122°E,27°~40°N)、北太平洋(170°E~170°W,27°~40°N)上空进行了对比。结果表明:高原上空气溶胶的体积密度、面积密度受Pinatubo火山喷发的影响主要发生在1991—1995年,然而气溶胶数密度受火山影响则不如前二者明显;高原上空气溶胶在对流层顶附近存在一个极大值区,在夏季该极大值区位于对流层顶下方(约120 hPa),而其他季节则位于对流层顶上方(约100hPa);青藏高原、中国东部地区、北太平洋三地上空气溶胶数密度的差异主要出现在60 hPa以下的气层,夏季差异最突出,高原上120 hPa附近的气溶胶数密度约为平原上的1.8倍,约为海洋上的5.5倍;在高原上空对流层顶附近以及平流层低层,气溶胶数密度与臭氧体积混合比呈很好的负相关关系,而在20 hPa以上则有明显的正相关关系;对比三地上空气溶胶与臭氧的关系,得到在对流层顶附近及平流层低层气溶胶在高原和平原上空与臭氧的变化呈很好的负相关,其中以高原上空的负相关关系更好,但是在海洋上空气溶胶和臭氧的相关不明显。而在20 hPa以上气层中,三地上空的气溶胶与臭氧的变化都具有很好的正相关关系。  相似文献   

6.
青藏高原平流层臭氧和气溶胶的变化趋势研究   总被引:2,自引:1,他引:2  
通过分析SAGEⅡ资料,发现青藏高原平流层臭氧存在递减趋势,15—50 km臭氧的变化对臭氧总量变化贡献最大,其中25—50 km和15—25 km两层的贡献大致相当。通过青藏高原和中国东部地区平流层臭氧变化的对比,清楚地看出:两地臭氧总量变化的差异主要是由于在15—25 km臭氧变化不同所致。5—7月臭氧变化趋势的情况与年平均的变化类似,两地臭氧变化的差异主要在平流层低层,即15—25 km。青藏高原平流层气溶胶面密度的时间变化序列显示:大的火山喷发对青藏高原平流层气溶胶具有重要影响,其影响可持续6年左右。从1997年至今,青藏高原18—25 km气溶胶面密度增加,最大的增长出现在23 km,每年大约增长4%—5%。而在16—17 km气溶胶的面密度出现减少趋势。与此同时,在37 km以下,青藏高原的温度出现递减的趋势,而且其递减速度比中国东部地区快;在37—50 km,温度出现增加的趋势,青藏高原的增温也比中国东部地区快。青藏高原平流层低层气溶胶的增加和温度的降低都将增强该区域非均相反应的作用。  相似文献   

7.
Long-term record of global distribution of ozone during 1979 to 2001, from Total Ozone Mapping Spectrometer (TOMS), over a tropical urban environment has been analyzed and compared with ground measurements. Increase in atmospheric UV-absorbing aerosol loading has been observed after 1991. TOMS columnar ozone during 1979 to 2001 suggested a clear Gaussian pattern of minimum concentration in winter months and maximum in summer months. TOMS ozone showed good correlation with the ground measured columnar ozone during winter months and negative correlation with Sunburning Ultraviolet (SUV) (280–370 nm), UVA and aerosol optical depth (AOD).  相似文献   

8.
We describe here a DIAL lidar system for atmospheric ozone measurements atAberystwyth, Wales, together witha method for deriving a stratospheric ozone profile from a single laserwavelength. Lidar measurements are used todepict the passage of three mesoscale ozone disturbances in the troposphereand stratosphere. In the troposphere, twosmall fold-like structures are shown beneath and at the edge of streamers ofhigh potential vorticity in ECMWFanalyses. MST radar measurements at the same time show that one of these foldswas actively turbulent, causingmixing of stratospheric and tropospheric air. In the stratosphere, a streamerof low-latitude air drawn into a filamentby a breaking Rossby wave event was observed crossing the lidar site.  相似文献   

9.
The data, measured by a three-wavelength Integrating Nephelometer over Lanzhou City during the winters of 2001/2002 and 2002/2003 respectively, have been analyzed for investigating the scattering properties of atmospheric aerosols and exploring their relationship and the status of air pollution. The aerosol particle volume distribution is inverted with the measured spectral scattering coefficients. The results show that the daily variation of the aerosol scattering coefficients is in a tri-peak shape. The average ratio of backscattering coefficient to total scattering coefficient at 550 nm is 0.158; there exists an excellent correlation between the scattering coefficients and the concentration of PM10. The average ratio of the concentration of PM10 to the scattering coefficients is 0.37 g m-2, which is contingent on the optical parameters of aerosol particles such as the size distribution, etc.; an algorithm is developed for inverting the volume distribution of aerosol particles by using the histogram and Monte-Carlo techniques, and the test results show that the inversion is reasonable.  相似文献   

10.
FY-3卫星上搭载的紫外臭氧总量探测仪(Total Ozone Unit,TOU)是我国首台自主研制的用于全球臭氧总量监测的仪器,自2008年5月至今已有3台仪器搭载在气象卫星(FY-3A/FY-3B/FY-3C)上成功发射并在轨运行。TOU利用紫外波段进行臭氧总量反演,以获得全球臭氧的分布及其变化。2013年,针对我国灰霾、沙尘等气溶胶污染事件频发的环境问题,TOU紫外探测数据被成功用于吸收性气溶胶指数(AAI)的反演,之后TOU被用于我国吸收性气溶胶污染事件的监测,为沙尘、灰霾等的预报提供监测数据。对TOU的数据和产品的质量和应用进行了介绍,包括L1B数据、臭氧总量产品及AAI指数。在此基础上,根据现有仪器的不足,对后续仪器的发展方向进行了阐述。  相似文献   

11.
Brewer 分光光度计遥感大气臭氧垂直廓线的研究   总被引:1,自引:0,他引:1       下载免费PDF全文
利用建立的球面分层大气散射模式,研究了Brewer仪器工作波长进行Umkehr短法反演所包含的信息量,给出Brewer仪器探测大气臭氧垂直廓线的方法。同时,用气溶胶光学厚度计算得到气溶胶订正系数,建立了Umkehr反演的程序,用此程序对TableMountain资料进行气溶胶修正,得到了较好的结果。对北京测站1991年1─3月资料进行由气溶胶造成的臭氧反演廓线的误差计算,结果表明,用常规反演方法得到的各层臭氧含量的误差与平流层气溶胶光学厚度有一近似线性的关系;进行气溶胶修正后,与国外的臭氧反演廓线的误差修正工作 ̄[1]比较,结果较一致。研究提出的气溶胶订正反演方法为更好地对平流层臭氧变化趋势进行研究提供了可能性和可靠的基础。  相似文献   

12.
The paper discusses the potential effects on the ozone layer of gases released by the engines of proposed high altitude supersonic aircraft. The major problem arises from the emissions of nitrogen oxides which have the potential to destroy significant quantities of ozone in the stratosphere. The magnitude of the perturbation is highly dependent on the cruise altitude of the aircraft. Furthermore, the depletion of ozone is substantially reduced when heterogeneous conversion of nitrogen oxides into nitric acid on sulfate aerosol particles is taken into account in the calculation. The sensitivity of the aerosol load on stratospheric ozone is investigated. First, the model indicates that the aerosol load induced by the SO2 released by aircraft is increased by about 10–20% above the background aerosols at mid-high latitude of the Northern Hemisphere at 15 km for the NASA emission scenario A (the NASA emission scenarios are explained in Tables I to III). This increase in aerosol has small effects on stratospheric ozone. Second, when the aerosol load is increased following a volcanic eruption similar to the eruption of El Chichon (Mexico, April 1982), the ozone column in spring increases by as much as 9% in response to the injection of NO x from the aircraft with the NASA emission scenario A. Finally, the modeled suggests that significant ozone depletion could result from the formation of additional polar stratospheric clouds produced by the injection of H2O and HNO3 by the aircraft engines.  相似文献   

13.
The data, measured by a three-wavelength Integrating Nephelometer over Lanzhou City during the winters of 2001/2002 and 2002/2003 respectively, have been analyzed for investigating the scattering properties of atmospheric aerosols and exploring their relationship and the status of air pollution. The aerosol particle volume distribution is inverted with the measured spectral scattering coefficients. The results show that the daily variation of the aerosol scattering coefficients is in a tri-peak shape. The average ratio of backscattering coefficient to total scattering coefficient at 550 nm is 0.158; there exists an excellent correlation between the scattering coefficients and the concentration of PM10. The average ratio of the concentration of PM10 to the scattering coefficients is 0.37g m^-2, which is contingent on the optical parameters of aerosol particles such as the size distribution, etc.; an algorithm is developed for inverting the volume distribution of aerosol particles by using the histogram and Monte-Carlo techniques, and the test results show that the inversion is reasonable.  相似文献   

14.
A two-step method is employed in this study to retrieve vertical ozone profiles using scattered measure- ments from the limb of the atmosphere. The combination of the Differential Optical Absorption Spectroscopy (DOAS) and the Multiplicative Algebraic Reconstruction Technique (MART) is proposed. First, the limb radiance, measured over a range of tangent heights, is processed using the DOAS technique to recover the effective column densities of atmospheric ozone. Second, these effective column densities along the lines of sight (LOSs) are inverted using the MART coupled with a forward model SCIATRAN (radiative transfer model for SCIAMACHY) to derive the ozone profiles. This method is applied to Optical Spectrograph and Infra Red Imager System (OSIRIS) radiance, using the wavelength windows 571-617 nm. Vertical ozone profiles between 10 and 48 km are derived with a vertical resolution of 1 km. The results illustrate a good agreement with the cloud-free coincident SCanning Imaging Absorption spectroMeter for Atmospheric CHartographY (SCIAMACHY) ozone measurements, with deviations less than ± 10% ( ± 5% for altitudes from 17 to 47 km). Furthermore, sensitivities of retrieved ozone to aerosol, cloud parameters and NO 2 concentration are also investigated.  相似文献   

15.
长三角工业区夏季近地层臭氧和颗粒物污染相互关系研究   总被引:4,自引:0,他引:4  
利用2013年5月15日到8月31日南京江北工业区(长三角典型工业区)同步的观测资料分析了近地层臭氧(O3)和细颗粒物(PM2.5)、气溶胶光学厚度(AOD)的变化特征及相互间的关系,并结合光化学箱模式分析了AOD对近地层O3生成的影响。结果表明,观测期间PM2.5平均质量浓度为56.2±20.1 μg m-3;AOD(500 nm)均值为1.4±0.9;波长指数α(440~870 nm)均值为1.0±0.3。PM2.5质量浓度24 h均值超国家二级标准20.2%,超标时AOD均值增加14.7%,α平均值增加23.9%,O3体积分数均值减少12.3%。O3超国家二级标准10.1%,超标时段AOD增加34.9%,α变化不显著。高温低湿条件下,O3日变化峰值(y)和PM2.5质量浓度(x)存在较高的线性相关。相对湿度<60%时,两者拟合曲线为y=0.97x+43.96(拟合度R2=0.60),温度>32°C时,两者拟合方程为y=1.24x+30.61(R2=0.64)。夏季长三角工业区呈现高浓度O3与高浓度PM2.5叠加的大气复合污染。O3日变化峰值和AOD变化呈显著负相关。模拟结果显示,O3日变化峰值(y)和AOD(x)呈现极高的负相关[y=-34.28x+181.62,R2 = 0.93或y=220.62·exp (-x/3.17)-19.50,R2=0.99]。  相似文献   

16.
Surface erythemal UV radiation is mainly affected by total column ozone, aerosols, clouds, and solar zenith angle. The effect of ozone on the surface UV radiation has been explored many times in the previous studies due to the decrease of ozone layer. In this study, we calculated the effect of aerosols on the surface UV radiation as well as that of ozone using data acquired from Ozone Monitoring Instrument (OMI). First, ozone, aerosol optical depth (AOD), and surface erythemal UVB radiation measured from satellite are compared with those from ground measurements. The results showed that the comparison for ozone was good with r 2 of 0.92. For aerosol, there was difference between satellite measurements and surface measurements due to the insufficient information on aerosol in the retrieval algorithm. The r 2 for surface erythemal UV radiation was high (~0.94) but satellite measurements showed about 30% larger values than surface measurements on average by not considering the effect of absorbing aerosols in the retrieval process from satellite measurements. Radiative amplification factor (RAF) is used to access the effect of ozone and aerosol quantitatively. RAF for ozone was 0.97~1.49 with solar zenith angle. To evaluate the effect of aerosol on the surface UV radiation, only clear-sky pixel data were used and solar zenith angle and total column amount of ozone were fixed. Also, RAF for aerosol was assessed according to the single scattering albedo (SSA) of aerosols. The results showed that RAF for aerosol with smaller SSA (< 0.90) was larger than that for with larger SSA (> 0.90). The RAF for aerosol was 0.09~0.22 for the given conditions which was relatively small compared to that for ozone. However, considering the fact that aerosol optical depth can change largely in time and space while the total column amount of ozone does not change very much, it needs to include the effect of aerosol to predict the variations of surface UV radiation more correctly.  相似文献   

17.
比较分析了2017年南极中山站3种仪器测量地面太阳紫外B(UVB)波段和紫外A(UVA)波段的辐照度。以Brewer光谱仪测值为参考,国产宽波段FSUVB日射表在UVB(波段280~315 nm)的辐照度相对误差为(55±75)%,误差随大气臭氧总量的增加呈上升趋势,但在南极“臭氧洞”期间偏低。Yankee UVB宽波段日射表在UVB(波段280~320 nm)的辐照度相对误差为(-31±22)%;国产宽波段FSUVA日射表在UVA(波段315~400 nm)的辐照度相对误差为(23±5.9)%。太阳天顶角低于80°的晴天以Tropospheric Ultraviolet Visible(TUV)辐射模式计算结果为参考时,FSUVB,Yankee UVB和FSUVA辐照度的平均相对误差分别为(30±37)%,(-22±19)%和(27±6.4)%,而Brewer相对误差未超过3.5%。国产宽波段UV日射表测值偏高,反映出波长较长的杂散光对太阳辐照度测值影响明显。  相似文献   

18.
水文循环过程受气候变化与人类活动的共同作用,区分气候内部自然变率与人类活动作用于水循环贡献对于增加气候变化的理解非常重要。本研究利用近期发展的考虑地下水取用水与灌溉影响的全球陆气耦合模式进行数值模拟,基于最优指纹法分析探讨中国东部季风区黄河、淮河、海河、珠江、长江、松花江流域水循环变化(地表温度、降水、径流、蒸散发)及归因。结果表明:大部分流域的地表温度年际变化在1965~2005年间检测到包括温室气体气溶胶人为排放、臭氧与土地利用变化产生的外强迫效应,显示在长期对于地表温度起主要作用的可能为上述强迫;1965~2005年降水年际变化仅在淮河及长江下游检测到上述强迫效应,且在长江下游效应占主导。在1965~1984年间,地表温度的年际变化在海河流域检测到由于地下水取水灌溉产生的外强迫效应,并且该效应占主导。在1982~2005年径流年际变化中,在淮河、长江下游及黄河下游处检测到了由于温室气体排放、气溶胶人为排放、臭氧变化及土地利用变化等产生的外强迫效应但无法有效分离,显示该信号在这些地区可能不为主导效应;1982~2005年间的蒸散发年际变化在珠江、长江下游同样检测到了上述强迫效应,并且该效应在长江下游占主导效应。  相似文献   

19.
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.  相似文献   

20.
20世纪80年代中国地区大气气溶胶光学厚度的平均状况分析   总被引:29,自引:3,他引:29  
利用中国北京等 41个甲种日射站 1 979~ 1 990年太阳直接辐射日总量和日照时数等资料 ,配合同期 TOMS version - 7臭氧观测资料 ,反演了 41个站逐年、逐月 0 .75μm大气气溶胶的平均光学厚度值 (Aerosol Optical Depth,AOD) ,据此分析了 1 2 a来中国大气气溶胶的变化和时空平均分布特征。结果表明 :中国大气气溶胶光学厚度 AOD的多年平均分布是以四川盆地为中心向四周减少 ,南疆盆地和长江中游武汉附近为另两个大值中心 ;长江中下游大部分地区、山东半岛以及广东沿海等 ,AOD值亦较大 ;而东北大部、西北大部、云南和福建沿海等地 AOD较小。AOD各月平均分布有所不同。中国绝大部分地区春季 AOD值最大 ,最小值则各地不同。 1 979~ 1 990年 ,青藏高原、四川盆地西部、贵州北部、长江中下游大部分地区、山东半岛和南疆盆地西部等 ,AOD呈增长趋势。而东北地区、西北地区大部、云贵高原和广西西部以及华东沿海等地 AOD呈减小势态。中国地区 AOD的季节变化曲线大体可分为单峰、一峰一谷、两峰一谷和多峰等 4种类型  相似文献   

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