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Aerosol Characteristics at a High Altitude Location in Central Himalayas: Optical Properties and Radiative Forcing

机译:喜马拉雅中部高海拔地区的气溶胶特征:光学性质和辐射强迫

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摘要

Collocated measurements of the mass concentrations of aerosol black carbon (BC) and composite aerosols near the surface were carried out along with spectral aerosol optical depths (AODs) from a high altitude station, Manora Peak in Central Himalayas, during a comprehensive aerosol field campaign in December 2004. Despite being a pristine location in the Shivalik Ranges of Central Himalayas, and having a monthly mean AOD (at 500 nm) of 0.059 $\pm$ 0.033 (typical to this site), total suspended particulate (TSP) concentration was in the range 15 - 40 micro g m^(-3) (mean value 27.1 $\pm$ 8.3 micro g m^(-3)). Interestingly, aerosol BC had a mean concentration of 1.36 $\pm$ 0.99 micro g m^(-3), contributed to ~5.0 $\pm$ 1.3 % to the composite aerosol mass. This large abundance of BC is found to have linkages to the human activities in the adjoining valley and to the boundary layer dynamics. Consequently, the inferred single scattering albedo lies in the range of 0.87 to 0.94 (mean value 0.90 $\pm$ 0.03), indicating significant aerosol absorption. The estimated aerosol radiative forcing was as low as 4.2 W m^(-2) at the surface, +0.7 W m^(-2) at the top of the atmosphere, implying an atmospheric forcing of +4.9 W m^(-2). Though absolute value of the atmospheric forcing is quite small, which arises primarily from the very low AOD (or the column abundance of aerosols), the forcing efficiency (forcing per unit optical depth) was $\sim$88 W m^(-2), which is attributed to the high BC mass fraction.
机译:在一次全面的气溶胶田间运动中,对来自喜马拉雅中部马诺拉峰高空站的光谱气溶胶光学深度(AOD)进行了地表附近气溶胶黑碳(BC)和复合气溶胶的质量浓度的合并测量。 2004年12月。尽管位于喜马拉雅中部Shivalik山脉的原始位置,并且每月平均AOD(在500 nm处)为0.059 $ \ pm $ 0.033(此站点典型),但总悬浮颗粒物(TSP)浓度仍在范围15-40 micro gm ^(-3)(平均值27.1 $ \ pm $ 8.3 micro gm ^(-3))。有趣的是,气溶胶BC的平均浓度为1.36 $ \ pm $ 0.99 micro g m ^(-3),占复合气溶胶质量的〜5.0 $ \ pm $ 1.3%。人们发现大量的卑诗省与附近山谷的人类活动和边界层动力学有联系。因此,推断的单散射反照率在0.87至0.94的范围内(平均值0.90 $ \ pm $ 0.03),表明有显着的气溶胶吸收。估计的表面气溶胶辐射强迫低至4.2 W m ^(-2),在大气层顶部低至+0.7 W m ^(-2),这意味着大气强迫为+4.9 W m ^(-2) )。尽管大气强迫的绝对值很小,这主要是由于极低的AOD(或气溶胶的色谱柱丰度)引起的,但强迫效率(每单位光学深度的强迫)为$ \ sim $ 88 W m ^(-2) ,这归因于较高的BC质量分数。

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