首页> 外文期刊>Applied optics >TROPOSPHERIC AEROSOL EXTINCTION COEFFICIENT PROFILES DERIVED FROM SCANNING LIDAR MEASUREMENTS OVER TSUKUBA, JAPAN, FROM 1990 TO 1993
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TROPOSPHERIC AEROSOL EXTINCTION COEFFICIENT PROFILES DERIVED FROM SCANNING LIDAR MEASUREMENTS OVER TSUKUBA, JAPAN, FROM 1990 TO 1993

机译:1990年至1993年日本对筑波的扫描激光测量得出的对流气溶胶消光系数

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Mie scattering lidar was used to observe aerosol extinction coefficient profiles in the troposphere over Tsukuba (140 E, 36 N), Japan, for three years from March 1990 to February 1993, and data obtained in fair weather were analyzed. The lidar measurements were made by a vertical scanning mode to generate profiles of extinction coefficients from the lidar level to a 12-km altitude. The extinction coefficients were derived from the lidar signals using a two-component (air molecule and aerosol) lidar equation, in which the ratio of aerosol extinction to backscattering was assumed to be constant. Seasonal average profiles were derived from individual profiles. Three-year average profiles were also calculated and modeled using mathematical expressions. The model profile assumed (1) a constant extinction ratio in the atmospheric boundary layer (ABL), (2) an exponentially decreasing extinction ratio above the ABL, and (3) a constant extinction ratio in the upper troposphere where the extinction ratio can be defined as the ratio of the aerosol extinction coefficient to the air molecule extinction coefficient. The extinction ratios both in the ABL and in the upper troposphere and the scale height that was used to express the exponential decrease were used as three unknown parameters. Seasonal variation of optical thickness that was obtained by integrating extinction coefficients with height was also investigated. (C) 1996 Optical Society of America [References: 26]
机译:1990年3月至1993年2月的3年中,使用Mie散射激光雷达观察了日本筑波(140 E,36 N)对流层的气溶胶消光系数分布,并分析了在晴朗天气中获得的数据。通过垂直扫描模式进行激光雷达测量,以生成从激光雷达水平到12公里高度的消光系数曲线。消光系数是使用两组分(空气分子和气溶胶)激光雷达方程从激光雷达信号得出的,其中,气溶胶消光与反向散射的比率假定为常数。季节性平均资料来自个人资料。还使用数学表达式计算和建模了三年平均轮廓。模型剖面假定(1)大气边界层(ABL)中的消光比恒定,(2)在ABL之上的指数消光比呈指数下降,(3)对流层上的消光比恒定,此处的消光比可以为定义为气溶胶消光系数与空气分子消光系数之比。 ABL和对流层中的消光比以及用来表示指数下降的水垢高度被用作三个未知参数。还研究了通过将消光系数与高度集成而获得的光学厚度的季节性变化。 (C)1996年美国眼镜学会[参考文献:26]

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