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1.
基于国际大气化学-气候模式比较计划模式数据评估中国沙尘气溶胶直接辐射强迫 总被引：2，自引：0，他引：2
目前气候模式对沙尘气溶胶直接辐射强迫模拟仍有很大不确定性,多模式对比有助于定量评估不确定范围。国际大气化学—气候模式比较计划（Atmospheric Chemistry and Climate Model Intercomparison Project,ACCMIP）旨在评估当前模式对短寿命大气成分辐射强迫和气候效应的模拟能力。基于7个ACCMIP模式模拟的中国地区沙尘气溶胶浓度,我们评估了中国区域沙尘气溶胶直接辐射强迫和不确定性范围。结果显示,中国区域沙尘气溶胶年排放总量为215±163 Tg a-1,区域年均地表浓度为41±27 μg m-3,柱浓度为9±4 kg m-2,光学厚度为0.09±0.05。中国区域年均沙尘气溶胶产生的大气顶短波、长波和总辐射强迫分别为-1.3±0.8 W m-2、0.7±0.4 W m-2和-0.5±0.7 W m-2;地表短波、长波和总的辐射强迫值为-1.5±1.0 W m-2、1.8±0.9 W m-2和0.2±0.2 W m-2。沙尘气溶胶长波辐射强迫对沙尘浓度的垂直分布敏感。高层沙尘气溶胶浓度越大,其在大气顶产生更强的正值长波辐射强迫。然而,沙尘气溶胶短波辐射强迫主要受整层沙尘柱浓度控制,对沙尘浓度的垂直分布较不敏感。本文结果可为中国沙尘气溶胶的气候模拟提供参考。 相似文献
2.
沙尘气溶胶辐射强迫全球分布的模拟研究 总被引：7，自引：2，他引：5
为了定景了解沙尘气溶胶对气候的影响,文中利用一个改进的辐射传输模式,结合伞球气溶胶数据集(G-ADS),计算了晴空条件下,冬夏两季沙尘气溶胶的直接辐射强迫在对流层顶和地面的全球分布,并讨论了云对沙尘气溶胶辐射强迫的影响.计算结果表明,对北半球冬季和夏季而言,在对流层顶沙尘气溶胶的全球短波辐射强迫的平均值分别为-0.477和-0.501 W/m2;长波辐射强迫分别为0.11和0.085 W/m2;全球平均短波地面辐射强迫冬夏两季分别为-1.362和-1.559 W/m2;长波辐射强迫分别为0.274和0.23 W/m2.沙尘气溶胶在对流层顶和地面的负辐射强迫的绝对值郁随太阳天顶角的余弦和地表反照率的增加而增大;地表反照率对沙尘气溶胶辐射强迫的强度和分布都有重要影响.研究指出:云对沙尘气溶胶的直接辐射强迫的影响不仅取决于云量,而且取决于云的高度和云水路径,以及地面反照率和太阳高度角等综合因素.中云和低云对沙尘气溶胶在对流层顶的短波辐射强迫的影响比高云明显.云的存在都使对流层顶长波辐射强迫减少,其中低云的影响最为明显.因此,在估算沙尘气溶胶总的直接辐射强迫时,云的贡献不可忽视. 相似文献
3.
沙尘气溶胶作为地球大气气溶胶的重要组成部分,对全球气候、生态环境和人体健康都有重要影响。厘清青藏高原地区的沙尘气溶胶时空分布变化,对研究青藏高原沙尘气溶胶气候环境效应有重要意义。利用风云卫星遥感资料、再分析资料等多源数据,统计分析了1999-2020年青藏高原上空沙尘气溶胶的时空分布特征。高原沙尘活动强度在季风期明显高于非季风期,沙尘气溶胶光学厚度（Dust Optical Depth, DOD）在春、夏、秋、冬季的多年平均分别为0.176、 0.064、 0.032、 0.060,气溶胶光学厚度（Aerosol Optical Depth, AOD）为0.223、 0.118、 0.069、 0.117。柴达木盆地是青藏高原地区沙尘活动最活跃的区域,在高原西部和南部监测到零星沙尘活动。2018-2020年,青藏高原上空发生沙尘事件的天数分别为：192天、 218天和212天。东亚地区沙尘源地（约62%）与中东、中亚地区沙尘源地（约30%）分别是高原北部和南部沙尘气溶胶的主要来源,源自北非地区的沙尘主要影响高原南部的高海拔地区。青藏高原地区沙尘活动在2000-2012年强度较高,201... 相似文献
4.
利用NCEP再分析资料和卫星观测资料,结合耦合了沙尘模块的中尺度模式WRF,通过个例分析研究了青藏高原及附近地区沙尘气溶胶从近地面向对流层上部和平流层下部传输的特征和机制以及青藏高原大地形对平流层与对流层之间物质交换的影响。结果表明,深对流活动可将近地面沙尘气溶胶传输到上对流层—下平流层区域,但是下平流层区域的沙尘气溶胶浓度分布依赖于地面沙尘源的位置和对流的强度,且与对流系统内是否有降水有关。在没有穿透性对流情况下,垂直上升运动不能直接将沙尘输送到下平流层,但上对流层的沙尘可通过扩散作用和小尺度的混合过程经过数小时缓慢地进入下平流层。在没有明显系统性降水的情况下,夏季青藏高原上空旺盛的对流活动和高地形使得高原上空成为气溶胶进入下平流层的主要区域。上对流层区域的沙尘气溶胶浓度还受到平流层空气入侵的影响,在没有强的地面沙尘排放源的情况下,平流层空气的入侵对上对流层区域气溶胶浓度的分布和演变有较大的影响。 相似文献
5.
黑碳气溶胶直接辐射强迫及其对中国夏季降水影响的模拟研究 总被引：8，自引：1，他引：7
利用NCAR的全球大气模式CAM3分析了黑碳气溶胶在大气顶和地表的直接辐射强迫分布及其季节变化,重点讨论了云对黑碳气溶胶直接辐射强迫的影响,以及黑碳气溶胶对中国夏季降水的影响。结果表明：黑碳气溶胶在大气顶和地表的直接辐射强迫分布范围和强度都具有明显的季节变化。有云条件下,黑碳气溶胶在大气顶产生正的直接辐射强迫,全球年平均强迫值为＋0.33 W·m－2;在地表产生负的直接辐射强迫,全球年平均强迫值为－0.56 W·m－2。晴空条件下,黑碳气溶胶在大气顶和地表的全球年平均辐射强迫值分别为＋0.21 和－0.71 W·m－2。云的存在对黑碳气溶胶的辐射强迫产生了很大的影响,使大气顶的正辐射强迫增加,地表的负辐射强迫减小。黑碳气溶胶导致夏季中国北方30°N～45°N之间区域降水明显增加;而中国长江以南地区除了海南和广西的部分城市外,降水明显减少。模拟结果表明,中国夏季近50年来经常发生的南涝北旱并非由黑碳气溶胶引起。 相似文献
6.
利用NCEP再分析资料和卫星观测资料,结合耦合了沙尘模块的中尺度模式WRF,通过个例分析研究了青藏高原及附近地区沙尘气溶胶从近地面向对流层上部和平流层下部传输的特征和机制以及青藏高原大地形对平流层与对流层之间物质交换的影响。结果表明,深对流活动可将近地面沙尘气溶胶传输到上对流层—下平流层区域,但是下平流层区域的沙尘气溶胶浓度分布依赖于地面沙尘源的位置和对流的强度,且与对流系统内是否有降水有关。在没有穿透性对流情况下,垂直上升运动不能直接将沙尘输送到下平流层,但上对流层的沙尘可通过扩散作用和小尺度的混合过程经过数小时缓慢地进入下平流层。在没有明显系统性降水的情况下,夏季青藏高原上空旺盛的对流活动和高地形使得高原上空成为气溶胶进入下平流层的主要区域。上对流层区域的沙尘气溶胶浓度还受到平流层空气入侵的影响,在没有强的地面沙尘排放源的情况下,平流层空气的入侵对上对流层区域气溶胶浓度的分布和演变有较大的影响。 相似文献
7.
《高原气象》2015,(4)
利用NCEP客观分析资料、卫星观测资料和中尺度化学模式(WRF-Chem),对2007年4月17日发生在青藏高原(下称高原)北侧塔克拉玛干沙漠地区的一次沙尘过程进行分析,研究了高原及附近地区沙尘气溶胶从地面向对流层上部和平流层下部传输的特征和机制,以及不同粒径沙尘粒子在传输中的差异。结果表明,沙尘粒子的垂直传输高度与背景水平风场的垂直分布特征密切相关,在没有云微物理过程参与的情况下,当高原上空出现深厚南北风交汇,形成穿透对流层顶的上升运动时,源于塔克拉玛干沙漠地区的沙尘气溶胶粒子,能到达高原上空,在辐合上升运动的作用下传输至下平流层,且具有明显的倾斜向上传输的特征。进一步分析表明,到达平流层下层的沙尘在空间上并不与地面沙尘源的位置相匹配。不同粒径的沙尘粒子的传输表现出不同的特征,粒径小的沙尘气溶胶粒子更容易在上升气流的作用下传至下平流层,而粒径8.0μm的沙尘粒子则在重力沉降作用影响下无法传至下平流层。敏感性数值试验结果表明,降低高原地形会使得高原上空沙尘气溶胶粒子向南和向上的传输变弱。 相似文献
8.
中国有机碳气溶胶时空分布与辐射强迫的模拟研究 总被引：4，自引：1，他引：3
利用区域气候模式RegCM3模拟研究2000年我国有机碳气溶胶的时空分布特征和辐射效应,得出以下结论:有机碳气溶胶主要分布在我国黄河以南、青藏高原以东的广大区域,且柱含量由南向北递减;柱含量最大值可达3 mg/m2以上,出现在华南、中南、云贵、四川和西藏东南部。另外,柱含量分布有着明显的季节性,冬季最大,春季次之,夏季最小。在此基础上,本文还对有机碳气溶胶的柱含量时空分布变化的原因进行了分析。有机碳气溶胶在大气顶和地表均产生负的辐射强迫,其分布特征与柱含量分布特征基本一致,而且大气顶和地表的辐射强迫都具有明显的季节变化。模拟的大气顶辐射强迫在-0.1～-0.5 W/m2之间,与IPCC估计的有机碳气溶胶的辐射强迫数值-0.41 W/m2相当,说明区域气候模式RegCM3中有关有机碳气溶胶的参数化方案是比较合理的。 相似文献
9.
《高原气象》2016,(3)
为了认识青藏高原严重沙漠化将产生的沙尘气溶胶及其影响,利用全球气溶胶气候模式CAM3.1对青藏高原沙漠化进行了敏感性模拟试验,进而探讨了高原沙漠对东亚大气气溶胶的最大可能贡献。结果表明,青藏高原上潜在的起沙源区主要分布在临近柴达木盆地的高原西部、藏南地区以及青南高原;高原起沙量春季最大,秋季次之,冬季第三,夏季最小。沙漠化的高原除了显著增加了高原上大气沙尘气溶胶的浓度,也显著增加了中国中西部地区近地面大气边界层的沙尘气溶胶浓度,远距离传输至中国中西部地区、东伸到达中国东海岸,甚至朝鲜半岛、日本直至太平洋上空对流层中部的沙尘气溶胶浓度同样增加明显。青藏高原沙源在近源区(即青藏高原及周边地区)的高贡献主要在低层,而在远源区(如日本岛南部海域及中太平洋区域)的贡献主要在高层。高原沙尘气溶胶极易被扬升到西风带,成为全球最高效率的沙尘远程传输源地。青藏高原沙漠化可能使其成为全球重要的沙尘气溶胶源地。 相似文献
10.
使用RegCM3-dust区域气候模式,单向嵌套MIROC3．2-hires全球模式输出结果,在IPCCA1B温室气体排放情景下,对中国及东亚地区进行了当代（1991年-2000年）和未来（2091年-2100年）水平分辨率为50km的气候以及沙尘气溶胶数值模拟试验。结果表明,模式对中国地区地面气温、降水和东亚沙尘气溶胶空间分布模拟较好。未来东亚沙尘气溶胶年平均起沙通量增加2％,其中12月-3月由于地表积雪量的减少而增加,4月-11月由于10m风速的减小而减少,不同强度的强起沙事件同样12月-3月增加,4月-11月减少。年平均沙尘气溶胶柱含量增加14％,其中3月-5月和8月略减少,其它月份增加。沙尘气溶胶引起地面（SRF）负辐射强迫和沙尘源区大气顶（TOA）正辐射强迫、下游地区TOA负辐射强迫,受沙尘气溶胶辐射强迫的影响,地面起沙通量和柱含量减少。 相似文献
11.
Estimation of the Aerosol Radiative Effect over the Tibetan Plateau Based on the Latest CALIPSO Product 总被引：2，自引：0，他引：2
Based on the CALIPSO (Cloud–Aerosol Lidar and Infrared Pathfinder Satellite Observation) Version 4.10 products released on 8 November 2016, the Level 2 (L2) aerosol product over the Tibetan Plateau (TP) is evaluated and the aerosol radiative effect is also estimated in this study. As there are still some missing aerosol data points in the daytime CALIPSO Version 4.10 L2 product, this study re-calculated the aerosol extinction coefficient to explore the aerosol radiative effect over the TP based on the CALIPSO Level 1 (L1) and CloudSat 2B-CLDCLASS-LIDAR products. The energy budget estimation obtained by using the AODs (aerosol optical depths) from calculated aerosol extinction coefficient as an input to a radiative transfer model shows better agreement with the Earth’s Radiant Energy System (CERES) and CloudSat 2B-FLXHR-LIDAR observations than that with the input of AODs from aerosol extinction coefficient from CALIPSO Version 4.10 L2 product. The radiative effect and heating rate of aerosols over the TP are further simulated by using the calculated aerosol extinction coefficient. The dust aerosols may heat the atmosphere by retaining the energy in the layer. The instantaneous heating rate can be as high as 5.5 K day–1 depending on the density of the dust layers. Overall, the dust aerosols significantly affect the radiative energy budget and thermodynamic structure of the air over the TP, mainly by altering the shortwave radiation budget. The significant influence of dust aerosols over the TP on the radiation budget may have important implications for investigating the atmospheric circulation and future regional and global climate. 相似文献
12.
黄土高原半干旱区典型日吸收性气溶胶综合观测分析 总被引：2，自引：0，他引：2
利用兰州大学半干旱气候与环境观测站的太阳光度计、激光雷达、微波辐射计综合观测资料,结合辐射传输模式分析了该地区秋季典型日2012年9月3~4日、21日和28日气溶胶物理特性、垂直分布特征,及其与气象条件的关系。研究时期的气溶胶主要为局地沙尘与人为污染混合气溶胶,吸收性明显,尺度较小。其中,4日西北风增强,远距离传输沙尘气溶胶,气溶胶光学厚度最大,粒子尺度明显增大。尝试利用灰色关联度法确定参考高度,分别为7.41 km、8.47 km、7.13 km和7.66 km,反演气溶胶消光系数,由此积分得到的光学厚度与太阳光度计观测值相关性可达0.975,反演效果较好。研究时期气溶胶的抬升主要受白天热力湍流作用,边界层发展,气溶胶向上传输,每日12时（当地时间,下同）至14时传输至最大高度,气溶胶抬升的高度对应大气加热率的高值区,低层加热率可达1 K d-1。气溶胶在大气层顶和地面造成负辐射强迫,分别为-12.707 W m-2、-25.398 W m-2,大气中表现为正辐射强迫,为12.692 W m-2,大气层顶的辐射强迫对气溶胶的物理特性最为敏感,当气溶胶吸收性明显时,大气层顶的瞬时辐射强迫会出现正值。 相似文献
13.
Assuming spheroidal and spherical particle shapes for mineral dust aerosols, the effect of particle shape on dust aerosol optical depth retrievals, and subsequently on instantaneous shortwave direct radiative forcing (SWDRF) at the top of the atmosphere (TOA), is assessed based on Moderate Resolution Imaging Spectroradiometer (MODIS) data for a case study. Specifically, a simplified aerosol retrieval algorithm based on the principle of the Deep Blue aerosol retrieval method is employed to retrieve dust aerosol optical depths, and the Fu-Liou radiative transfer model is used to derive the instantaneous SWDRF of dust at the TOA for cloud-free conditions. Without considering the effect of particle shape on dust aerosol optical depth retrievals, the effect of particle shape on the scattering properties of dust aerosols (e.g., extinction efficiency, single scattering albedo and asymmetry factor) is negligible, which can lead to a relative difference of at most 5% for the SWDRF at the TOA. However, the effect of particle shape on the SWDRF cannot be neglected provided that the effect of particle shape on dust aerosol optical depth retrievals is also taken into account for SWDRF calculations. The corresponding results in an instantaneous case study show that the relative differences of the SWDRF at the TOA between spheroids and spheres depend critically on the scattering angles at which dust aerosol optical depths are retrieved, and can be up to 40% for low dust-loading conditions. 相似文献
14.
Lee Wei-Liang Liou K. N. He Cenlin Liang Hsin-Chien Wang Tai-Chi Li Qinbin Liu Zhenxin Yue Qing 《Theoretical and Applied Climatology》2017,129(3-4):1373-1382
We investigate the snow albedo variation in spring over the southern Tibetan Plateau induced by the deposition of light-absorbing aerosols using remote sensing data from moderate resolution imaging spectroradiometer (MODIS) aboard Terra satellite during 2001–2012. We have selected pixels with 100 % snow cover for the entire period in March and April to avoid albedo contamination by other types of land surfaces. A model simulation using GEOS-Chem shows that aerosol optical depth (AOD) is a good indicator for black carbon and dust deposition on snow over the southern Tibetan Plateau. The monthly means of satellite-retrieved land surface temperature (LST) and AOD over 100 % snow-covered pixels during the 12 years are used in multiple linear regression analysis to derive the empirical relationship between snow albedo and these variables. Along with the LST effect, AOD is shown to be an important factor contributing to snow albedo reduction. We illustrate through statistical analysis that a 1-K increase in LST and a 0.1 increase in AOD indicate decreases in snow albedo by 0.75 and 2.1 % in the southern Tibetan Plateau, corresponding to local shortwave radiative forcing of 1.5 and 4.2 W m−2, respectively.
相似文献15.
Current global climate models cannot resolve the complex topography over the Tibetan Plateau (TP) due to their coarse resolution. This study investigates the impacts of horizontal resolution on simulating aerosol and its direct radiative effect (DRE) over the TP by applying two horizontal resolutions of about 100 km and 25 km to the Chinese Academy of Sciences Flexible Global Ocean-Atmosphere Land System (CAS FGOALS-f3) over a 10-year period. Compared to the AErosol RObotic NETwork observations, a high-resolution model (HRM) can better reproduce the spatial distribution and seasonal cycles of aerosol optical depth (AOD) compared to a low-resolution model (LRM). The HRM bias and RMSE of AOD decreased by 0.08 and 0.12, and the correlation coefficient increased by 0.22 compared to the LRM. An LRM is not sufficient to reproduce the aerosol variations associated with fine-scale topographic forcing, such as in the eastern marginal region of the TP. The difference between hydrophilic aerosols in an HRM and LRM is caused by the divergence of the simulated relative humidity (RH). More reasonable distributions and variations of RH are conducive to simulating hydrophilic aerosols. An increase of the 10-m wind speed in winter by an HRM leads to increased dust emissions. The simulated aerosol DREs at the top of the atmosphere (TOA) and at the surface by the HRM are –0.76 W m–2 and –8.72 W m–2 over the TP, respectively. Both resolution models can capture the key feature that dust TOA DRE transitions from positive in spring to negative in the other seasons. 相似文献
16.
Influences of the mixing treatments of anthropogenic aerosols on their effective radiative forcing (ERF) and global aridity are evaluated by using the BCC_AGCM2.0_CUACE/Aero, an aerosol–climate online coupled model. Simulations show that the negative ERF due to external mixing (EM, a scheme in which all aerosol particles are treated as independent spheres formed by single substance) aerosols is largely reduced by the partial internal mixing (PIM, a scheme in which some of the aerosol particles are formed by one absorptive and one scattering substance) method. Compared to EM, PIM aerosols have much stronger absorptive ability and generally weaker hygroscopicity, which would lead to changes in radiative forcing, hence to climate. For the global mean values, the ERFs due to anthropogenic aerosols since the pre-industrial are–1.02 and–1.68 W m–2 for PIM and EM schemes, respectively. The variables related to aridity such as global mean temperature, net radiation flux at the surface, and the potential evaporation capacity are all decreased by 2.18/1.61 K, 5.06/3.90 W m–2, and 0.21/0.14 mm day–1 since 1850 for EM and PIM schemes, respectively. According to the changes in aridity index, the anthropogenic aerosols have caused general humidification over central Asia, South America, Africa, and Australia, but great aridification over eastern China and the Tibetan Plateau since the pre-industrial in both mixing schemes. However, the aridification is considerably alleviated in China, but intensified in the Arabian Peninsula and East Africa in the PIM scheme. 相似文献
17.
在过去的20多年里,中外对硫酸盐气溶胶做了大量的研究,对它在大气中的排放、含量、光学特征和辐射强迫有了深入的认识;由于硝酸盐气溶胶在大气中平均含量比硫酸盐低很多,因此过去人们对硝酸盐的研究没有给予重视。然而,近年来的研究表明,硝酸盐气溶胶的散射性质在某些波段甚至强于硫酸盐;同时,由于未来对人为硫酸盐前体物的减排,硫酸盐气溶胶排放会大幅度减少,而硝酸盐气溶胶的排放却增长迅速,其在人为气溶胶中所占的比重越来越高,将会导致其在未来造成的辐射强迫有可能超过硫酸盐,使得其在地区范围内和季节尺度上成为重要的辐射强迫和气候影响因子。中国是硝酸盐气溶胶排放量较大的地区,硝酸盐对未来中国气候和气候变化的影响显得越来越重要。因此,就近年来有关硝酸盐气溶胶的排放和在大气中的浓度变化、光学厚度分布特征及其辐射强迫的研究进展做了回顾和介绍,并对其未来的研究做了展望。 相似文献
18.
平流层气溶胶的辐射强迫及其气候响应的水平二维分析 总被引：7，自引：0，他引：7
利用比较先进的辐射模式计算了平流层气溶胶的辐射强迫,并对之进行了参数化。结果发现平流层气溶胶的辐射强迫的水平分布不仅与其本身的水平变化有关,而且与下垫面的反照率有很大的关系。利用近期开发的二维能量平衡模式模拟了皮纳图博火山气溶胶对地面平衡温度的影响,结果表明:皮纳图博火山至喷发后1年半左右降温达最大,至喷发后第5年降温已很小。 相似文献
19.
Muhammad Ali Salman Tariq Khalid Mahmood Asim Daud Adila Batool Zia-ul-Haq 《Asia-Pacific Journal of Atmospheric Sciences》2014,50(2):153-162
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. 相似文献