日本地球惑星科学連合2016年大会

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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-AS12] 大気化学

2016年5月25日(水) 15:30 〜 17:00 303 (3F)

コンビーナ:*入江 仁士(千葉大学環境リモートセンシング研究センター)、町田 敏暢(国立環境研究所)、谷本 浩志(国立環境研究所)、岩本 洋子(東京理科大学 理学部第一部)、座長:笹川 基樹(独立行政法人国立環境研究所)、Sasakawa Motoki(NIES National Institute of Environmental Studies)、松井 仁志(名古屋大学大学院環境学研究科)

15:45 〜 16:00

[AAS12-08] スバルバール諸島ニーオルスンにおける大気主成分濃度・同位体比の観測から示唆される下層大気の分子拡散分離

*石戸谷 重之1後藤 大輔2菅原 敏3森本 真司4青木 周司4村山 昌平1中澤 高清4 (1.産業技術総合研究所、2.国立極地研究所、3.宮城教育大学、4.東北大学)

キーワード:大気成分拡散分離、Ar/N2比、主成分同位体比、気温逆転層

Recent technical advances has made it possible to observe a molecular diffusive separation of the atmosphere based on high precision measurements of the composition of atmospheric major components. In the middle to lower stratosphere, Ishidoya et al. (2013) reported the existence of observable gravitational separation based on the measurements of stratospheric air samples collected using a balloon-borne cryogenic air sampler. In the lower atmosphere, Adachi et al. (2006) reported the diffusive separation of Ar and N2, mainly due to thermal diffusion, in the center of a wide desert during the nighttime when vertical temperature inversions are generated. To examine whether the diffusive separation of the atmosphere is also detectable near the surface in polar region, air samples collected at Ny-Ålesund, Svalbard (79°N, 12°E) have been analyzed for delta(Ar/N2), delta(O2/N2), delta15N of N2, delta18O of O2 and delta40Ar by using a mass spectrometer (Ishidoya and Murayama, 2014) since January 2013. It was found that delta15N and delta18O show small but significant seasonal cycles, with the seasonal maxima and minima in winter and summer, respectively. The peak-to-peak amplitudes of the respective seasonal cycles of delta15N and delta18O were about 2 and 4 per meg. On the other hand, no significant seasonal cycle was seen in delta(Ar/N2). If we assume the seasonal cycles of delta15N and delta18O are attributed mainly to gravitational separation in a temperature inversion layer during polar night in winter and corrected the delta(Ar/N2) for the separation by subtracting 12 x (delta15N + delta18O/2)/2 (delta(Ar/N2)cor), then the delta(Ar/N2)cor show clear seasonal cycle with a maximum in August. The peak-to-peak amplitude of the seasonal delta(Ar/N2)cor cycle is about 25 per meg, and the appearance time of seasonal maximum agrees with that of the sea surface temperature around Ny-Ålesund. These results suggest that gravitational separation is observable near the surface at Ny-Ålesund. Our suggestion would be supported by Keeling et al. (2004) who reported the delta(Ar/N2) observed in the polar region may be detectably enriched near the ground by gravitational separation or thermal diffusion under condition of strong surface inversions.

References
Adachi, Y. et al. (2006) Diffusive separation of the lower atmosphere, Science, 311, 1429.
Ishidoya, S. et al. (2013) Gravitational separation in the stratosphere – a new indicator of atmospheric circulation. Atmos. Chem. Phys., 13, 8787–8796, www.atmos-chem-phys.net/13/8787/2013/, doi:10.5194/acp-13-8787-2013.
Ishidoya, S. & Murayama, S. (2014) Development of high precision continuous measuring system of the atmospheric O2/N2 and Ar/N2 ratios and its application to the observation in Tsukuba, Japan. Tellus B, 66, 22574, http://dx.doi.org/ 10.3402/tellusb.v66.22574.
Keeling, R. F. et al. (2004) Measurement of changes in atmospheric Ar/N2 ratio using a rapid-switching, single-capillary mass spectrometer system, Tellus B, 56, 322–338.