日本地球惑星科学連合2019年大会

講演情報

[J] ポスター発表

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-AS04] 大気化学

2019年5月30日(木) 17:15 〜 18:30 ポスター会場 (幕張メッセ国際展示場 8ホール)

コンビーナ:中山 智喜(長崎大学 大学院水産・環境科学総合研究科)、岩本 洋子(広島大学 生物圏科学研究科)、豊田 栄(東京工業大学物質理工学院)、江口 菜穂(Kyushu University)

[AAS04-P31] 気象庁観測所において観測された大気中ラドン濃度の変動

*石島 健太郎1坪井 一寛1松枝 秀和1澤 庸介1丹羽 洋介2,1眞木 貴史1中村 貴3 (1.気象研究所、2.国立環境研究所、3.気象庁)

キーワード:ラドン、GSAM-TM

Japan Meteorological Agency (JMA) has been operating several stations to monitor atmospheric greenhouse gases since the late 1980s under the Global Atmosphere Watch programme of the World Meteorological Organization (WMO/GAW). They show synoptic, seasonal, interannual variations, and trends due to changes in atmospheric transport and source/sink strength. To know their transport from land regions, we started the monitoring of atmospheric Radon-222 (222Rn) in the 2000s at the JMA stations. Because 222Rn is emitted from almost only lands and chemically inert, it is useful to identify temporal variability of atmospheric greenhouse gases due to sources/sinks on land. 222Rn also radioactively decays with the half-life of 3.8 days, so is widely utilized to validate regional transport of atmospheric transport model through the model-observation comparisons. Understanding such transport process is also supported by using an atmospheric transport model. We have just started to use a newly developed on-line atmospheric tracer transport model (GSAM-TM). The tracer transport process is driven by a low-resolution version (TL95) of JMA's operational global numerical weather prediction model (GSAM).
In this study, we analyze the observed and model simulated atmospheric 222Rn concentration, to understand the transport process of land-origin atmospheric tracer as well as to validate the GSAM-TM. For example, the model well reproduces high 222Rn peaks, which are frequently observed at Minamitorishima (MNM; 24.28°N, 153.98°E) and Chichijima (CCJ; 27.09°N, 142.19°E) in winter to spring. Especially in winter, there are many cases that a high peak is first observed at CCJ and one day after at MNM. They are mainly produced by a cold front moving eastward with dense 222Rn behind the frontal line. The peak height at MNM is about two-thirds of that at CCJ. It is slightly smaller than that expected from decay by the 3.8 days half-life (about four-fifths), because dense 222Rn trapped by the front is diluted mainly by diffusion while transported. The model also well reproduces such peak attenuation degree. More details and results of 222Rn-age tracer simulations as well as of other JMA station will also be discussed in our presentation.

Acknowledgements. We sincerely thank all members of the JMA for operating 222Rn measurement systems at JMA monitoring stations