Polar vortex meandering and stratospheric aerosol distribution: Lidar measurements at Fairbanks, Alaska (scientific paper)

Iwasaka, Yasunobu, Shibata, Takashi, Adachi, Hiroshi, Sakai, Tetsu, Ojio, Teturo, Fujiwara, Motowo, Shiraishi, Koichi, Miyagawa-Kondoh, Koji, Nakane, Hideki
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引用次数: 1

Abstract

Lidar measurements at Fairbanks, Alaska (64°49' N, 147°52' W) and Ny-Aalesund, Norway (78°54'N, 11°53'E) in December 1991 and January, 1994, respectively, was made to monitor distribution of stratospheric aerosols. The location of Fairbanks lidar site is advantageous to see the effect of polar vortex wall to stratospheric aerosol density distribution since the lidar site is near the polar vortex wall, and sometimes inside and sometimes outside of the polar vortex owing meandering motion of polar vortex. Lidar site of Ny-Aalesund is usually inside of the polar vortex in winter. Comparison of measurements at Fairbanks and Ny-Aalesund showed that polar vortex meandering disturbed profiles of stratospheric aerosol content. Comparing measurements at Fairbanks and Toyokawa, Japan (34°45' N, 137°24' E) the measurements at Fairbanks are well corresponding to the long tens trend observed at Toyokawa, and noticeable day-to-day variations in aerosol content, integrated backscattering coefficient of stratospheric particulate matter, in winter of 1993/1994, which possibly due to the polar atmospheric effect, are detected in the Fairbanks data. Above about 20 km there was little aerosol content when the lidar station was inside of polar vortex. Large enhancement of aerosol load near the local tropopause was observed, which may associate with aerosol descending from the stratosphere to the troposphere near the wall of polar vortex.
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极地涡旋蜿蜒和平流层气溶胶分布:阿拉斯加费尔班克斯的激光雷达测量(科学论文)
分别于1991年12月和1994年1月在阿拉斯加费尔班克斯(北纬64°49′,西经147°52′)和挪威新奥勒松(北纬78°54′,东经11°53′)进行了激光雷达测量,以监测平流层气溶胶的分布。由于Fairbanks激光雷达站点靠近极涡壁,且由于极涡的蜿蜒运动时而在极涡内时而在极涡外,因此有利于观测极涡壁对平流层气溶胶密度分布的影响。冬季新奥勒松的激光雷达站点通常位于极地涡旋内部。费尔班克斯和新奥勒松测量值的比较表明,极地涡旋的蜿蜒扰动了平流层气溶胶含量的剖面。比较在费尔班克斯和日本丰川(北纬34°45′,东经137°24′)的测量结果,费尔班克斯的测量结果与在丰川观测到的长10年趋势非常吻合,并且在1993/1994年冬季,在费尔班克斯的数据中发现了气溶胶含量、平流层颗粒物综合后向散射系数的显著逐日变化,这可能是由于极地大气效应造成的。当激光雷达站处于极涡内部时,20 km以上的气溶胶含量很少。在局地对流层顶附近观测到气溶胶负荷的大幅增强,这可能与气溶胶从平流层下降到极地涡旋壁附近的对流层有关。
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