日本地球惑星科学連合2018年大会

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[EE] 口頭発表

セッション記号 A (大気水圏科学) » A-AS 大気科学・気象学・大気環境

[A-AS02] 大規模な水蒸気場と組織化した雲システム

2018年5月22日(火) 15:30 〜 17:00 301B (幕張メッセ国際会議場 3F)

コンビーナ:三浦 裕亮(国立大学法人 東京大学大学院 理学系研究科 地球惑星科学専攻)、濱田 篤(富山大学都市デザイン学部)、横井 覚(海洋研究開発機構、共同)、佐藤 正樹(東京大学大気海洋研究所)、座長:濱田 篤

15:45 〜 16:00

[AAS02-08] Characteristics of the Tropical Tropopause Inversion Layer using High-Resolution Temperature Profiles by COSMIC GPS-RO

*Noersomadi Noersomadi1Toshitaka Tsuda2Masatomo Fujiwara3 (1.Research Institute for Sustainable Humanosphere, Kyoto University, Japan; National Institute of Aeronautic and Space, Indonesia 、2.Research Institute for Sustainable Humanosphere, Kyoto University, Japan; Research Organization and Information System, Tokyo, Japan、3.Faculty of Environmental Earth Science, Hokkaido University, Japan)

キーワード:COSMIC, GPS-RO, Full Spectrum Inversion, Tropopause Inversion Layer

This study focuses on the sharp variations of the temperature structure near the cold point tropopause (CPT), which is called the tropopause inversion layer (TIL). We analyze the height variations of the Brunt-Väisälä frequency squared (N2) from the vertical gradient of the temperature data retrieved from the COSMIC GPS-RO in 2007-2016 using the Full Spectrum Inversion (cosmicfsi), which has the vertical resolution of about 0.1 km. This study describes new definition of tropical TIL utilizing high resolution of cosmicfsi that able to delineate the thin layer of static stability near tropopause. We examine the statistical distribution of the TIL parameters; such as S-aCPT, which is the difference between the maximum N2 above CPT (maxN2) and N2 at CPT, and S-bCPT, the difference between the minimum N2 below CPT (minN2) and N2 at CPT, the height difference distance for maxN2 and minN2 relative to CPT (dH-aCPT and dH-bCPT). The mean values of S-aCPT and S-bCPT are 6.2 × 10−4 s−2 and 4.0 × 10−4 s−2, respectively, and the standard deviation of S-aCPT is approximately three times larger than that for S-bCPT. The mean and standard deviation of both dH-aCPT and dH-bCPT are 0.4 ± 0.2 km and 0.5 ± 0.2 km, respectively. We find S-aCPT reached up to > 10 × 10−4 s−2 from its random frequency distribution and dH-aCPT was mostly < 0.5 km, indicating a very sharp thermal gradient due to very low temperature. We also discuss the TIL depth (dH) which is defined as height difference at N2 equal to 80% of maxN2.