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Raman lidar measurements of the aerosol extinction-to-backscatter ratio over the Southern Great Plains

机译:拉曼激光雷达对大平原南部气溶胶消光与后向散射比的测量

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We derive profiles of the aerosol extinction-to-backscatter ratio, S-a, at 355 nm using aerosol extinction and backscatter profiles measured during 1998 and 1999 by the operational Raman lidar at the Department of Energy Atmospheric Radiation Measurement Program Southern Great Plains site in north central Oklahoma. Data from this Raman/Rayleigh-Mie lidar, which measures Raman scattering from nitrogen as well as the combined molecular (Rayleigh) and aerosol (Mie) scattering at the laser wavelength, are used to derive aerosol extinction and backscattering independently as a function of altitude. Because this lidar operates at 355 nm, where molecular backscattering is comparable to aerosol backscattering, S-a retrievals are generally limited to conditions where aerosol extinction at 355 nm is >0.03 km(-1). The mean value of S-a at 355 nm derived for this period was 68 sr with a standard deviation of 12 sr. S-a was generally about 5-10 sr higher during high aerosol optical thickness (AOT) (>0.3) conditions than during low AOT (<0.1). A similar increase in S-a was found when the relative humidity increased from 30 to 80%. Large (> 15%) variations in the vertical profile of S-a occurred about 30% of the time, which implies that significant variability in the vertical distribution of the aerosol size distribution, shape, and/or composition often occurs. The Raman lidar measurements of S-a were compared with estimates of particle size and refractive index derived from an algorithm that uses ground-based Sun photometer measurements of Sun and sky radiance. For 17 cases of coincident Raman lidar and Sun and sky radiance measurements, S-a was linearly correlated with the aerosol fine mode effective radius and the volume ratio of fine/coarse particles. [References: 57]
机译:我们使用能源部大气辐射测量计划南部大平原地区北部中部能源大气辐射测量计划的运行拉曼激光雷达在1998年和1999年期间测量的气溶胶消光和反向散射剖面,得出了355 nm处的气溶胶消退与反向散射比Sa的剖面。俄克拉荷马州。来自此拉曼/瑞利-米德激光雷达的数据用于测量氮气中的拉曼散射以及激光波长处的分子(瑞利)和气溶胶(米氏)组合散射,可用于根据高度独立地得出气溶胶的消光和反向散射。由于此激光雷达在355 nm处工作,分子反向散射可与气溶胶反向散射相媲美,因此S-a检索通常限于355 nm处气溶胶消光> 0.03 km(-1)的条件。在此期间得出的355 nm处S-a的平均值为68 sr,标准偏差为12 sr。通常,在高气溶胶光学厚度(AOT)(> 0.3)条件下,S-a比低AOT(<0.1)高约5-10 sr。当相对湿度从30%增加到80%时,S-a也有类似的增加。 S-a垂直剖面的大变化(> 15%)发生在大约30%的时间,这意味着气溶胶尺寸分布,形状和/或成分的垂直分布经常发生显着变化。将S-a的拉曼激光雷达测量结果与通过使用基于地面的太阳光度计测量太阳和天空辐射率的算法得出的粒径和折射率估算值进行了比较。对于同时进行拉曼激光雷达和太阳与天空辐射测量的17个案例,S-a与气溶胶细模有效半径和细/粗颗粒的体积比线性相关。 [参考:57]

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