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首页> 外文期刊>Journal of Geophysical Research, D. Atmospheres: JGR >Comparisons of aerosol optical depth and surface shortwave irradiance and their effect on the aerosol surface radiative forcing estimation
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Comparisons of aerosol optical depth and surface shortwave irradiance and their effect on the aerosol surface radiative forcing estimation

机译:气溶胶光学深度和表面短波辐照度的比较及其对气溶胶表面辐射强迫估算的影响

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Column aerosol optical depth (AOD) and surface shortwave irradiance (SSI) measurements relevant to computation of the aerosol surface radiative forcing (ΔF) and forcing efficiency (β) were taken as part of Aerosol Characterization Experiment-Asia (ACE-Asia) at the Gosan surface site in Korea in April 2001. We compare the AOD and SSI derived from three different types of Sun photometers and three sets of radiometers. We also estimate the ΔF and β using two methods and quantify the observational uncertainties of these parameters. A comparison of the AOD at 500 nm shows that the three Sun photometers generally agreed within 0.014 (mean), 0.0142 (bias), and 0.0298 (root mean square) for coincident observations. Over the course of the comparison, the mean differences between the SSI measurements were 1.6, 11.7, and 10.1 Wm?2 for direct, diffuse and global irradiances, respectively. However, for both the AOD and the SSI comparisons, relatively high instantaneous differences between the instruments were apparent on days with heavy dust at the surface. The mean β and associated deviations, which were estimated by the combinations of different instrument-derived AODs and SSIs, for simultaneous observation data at a 60° solar zenith angle are ?79.50 ± 3.92 and ?82.57 ± 5.70 Wm?2/τ500 for globalshaded (sum of direct and diffuse irradiances) and globalunshaded (measured by the unshaded pyranometer) irradiances, respectively. The uncertainties in β associated with uncertainties in the AOD and SSI (in parentheses) for globalshaded and globalunshaded irradiance are about 8.6% and 3.2% (10.7%), respectively. A 2% difference between the measured global irradiances for a given 9 days was translated into an uncertainty of 19% in ΔF. This difference in ΔF between instruments caused a 14% deviation in β.
机译:与气溶胶表面辐射强迫(ΔF)和强迫效率(β)的计算相关的柱气溶胶光学深度(AOD)和表面短波辐照度(SSI)测量被作为亚洲气溶胶表征实验(ACE-Asia)的一部分2001年4月在韩国的Gosan地面站点。我们比较了三种不同类型的太阳光度计和三套辐射度计得出的AOD和SSI。我们还使用两种方法估计ΔF和β,并量化这些参数的观测不确定性。在500 nm处AOD的比较表明,对于同时进行的观测,这三种Sun光度计通常在0.014(均值),0.0142(偏置)和0.0298(均方根)之间一致。在比较过程中,直接,漫射和整体辐照度的SSI测量值之间的平均差分别为1.6、11.7和10.1 Wm?2。但是,对于AOD和SSI两者的比较,仪器之间的相对较高的瞬时差异在表面积有大量灰尘的日子很明显。对于全遮光罩,在60°太阳天顶角的同时观测数据,通过不同仪器衍生的AOD和SSI的组合估算的平均β和相关偏差分别为?79.50±3.92和?82.57±5.70 Wm?2 /τ500 (直接和漫射辐照度的总和)和全局未遮罩(由未遮挡的日射强度计测量)的辐照度。对于整体阴影辐照度和整体非阴影辐照度,β的不确定性与AOD和SSI的不确定性(在括号中)分别约为8.6%和3.2%(10.7%)。在给定的9天中测得的全球辐照度之间的2%的差异转化为ΔF的19%的不确定度。仪器之间的ΔF差异导致β偏差14%。

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