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首页> 外文期刊>Journal of Geophysical Research, D. Atmospheres: JGR >Determining the contribution of volcanic ash and boundary layer aerosol in backscatter lidar returns: A three-component atmosphere approach
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Determining the contribution of volcanic ash and boundary layer aerosol in backscatter lidar returns: A three-component atmosphere approach

机译:确定火山灰和边界层气溶胶在后向散射激光雷达回波中的作用:三成分大气法

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[1] A solution of the lidar equation is discussed, that permits combining backscatter and depolarization measurements to quantitatively distinguish two different aerosol types with different depolarization properties. The method has been successfully applied to simultaneous observations of volcanic ash and boundary layer aerosol obtained in Exeter, United Kingdom, on 16 and 18 April 2010, permitting the contribution of the two aerosols to be quantified separately. First a subset of the atmospheric profiles is used where the two aerosol types belong to clearly distinguished layers, for the purpose of characterizing the ash in terms of lidar ratio and depolarization. These quantities are then used in a three-component atmosphere solution scheme of the lidar equation applied to the full data set, in order to compute the optical properties of both aerosol types separately. On 16 April a thin ash layer, 100-400 m deep, is observed (average and maximum estimated ash optical depth: 0.11 and 0.2); it descends from ~2800 to ~1400 m altitude over a 6-hour period. On 18 April a double ash layer, ~400 m deep, is observed just above the morning boundary layer(average and maximum estimated ash optical depth: 0.19 and 0.27). In the afternoon the ash is entrained into the boundary layer, and the latter reaches a depth of ~1800 m(average and maximum estimated ash optical depth: 0.1 and 0.15). An additional ash layer, with a very small optical depth, was observed on 18 April at an altitude of 3500-4000 m. By converting the lidar optical measurements using estimates of volcanic ash specific extinction, derived from other works, the observations seem to suggest approximate peak ash concentrations of ~1500 and ~1000 g/m3, respectively, on the two observations dates.
机译:[1]讨论了激光雷达方程的解决方案,该解决方案允许结合反向散射和去极化测量来定量地区分具有不同去极化特性的两种不同气溶胶类型。该方法已成功应用于2010年4月16日至18日在英国埃克塞特获得的火山灰和边界层气溶胶的同时观测,这两种气溶胶的贡献可以分别量化。首先,使用大气分布的子集,其中两种气溶胶类型属于明显不同的层,目的是根据激光雷达比和去极化来表征灰分。然后,将这些量用于应用于整个数据集的激光雷达方程的三组分大气溶液方案中,以便分别计算两种气溶胶类型的光学特性。在4月16日,观察到了一个薄的灰烬层,深100-400 m(平均灰烬光学最大深度和最大估计光学深度:0.11和0.2)。它在6小时内从〜2800下降到〜1400 m高度。 4月18日,在早晨边界层正上方发现了一个深约400 m的双灰层(平均和最大灰烬光学深度:0.19和0.27)。下午,灰烬被带入边界层,边界层的深度约为1800 m(灰烬平均光学平均深度和最大估计光学深度:0.1和0.15)。在4月18日,在3500-4000 m的高空观察到了另一个具有很小光学深度的灰层。通过使用从其他工作得出的火山灰比绝灭的估计值转换激光雷达光学测量结果,这些观察结果似乎表明在两个观察日期分别有大约1500和〜1000 g / m3的近似峰值灰分浓度。

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