日本地球惑星科学連合2024年大会

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[E] 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-AS03] 大規模な水蒸気場と組織化した雲システム

2024年5月29日(水) 10:45 〜 12:00 103 (幕張メッセ国際会議場)

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)、高須賀 大輔(東北大学大学院理学研究科)、濱田 篤(富山大学)、横井 覚(海洋研究開発機構)、座長: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)、高須賀 大輔(東京大学大気海洋研究所)

11:30 〜 11:45

[AAS03-10] Matching the weak temperature gradient and the quasi-geostrophic solutions in a shallow water model on a frictionless f-plane

*神山 翼1三浦 裕亮2 (1.お茶の水女子大学、2.東京大学)

キーワード:熱帯中緯度境界、弱温度勾配系、準地衡風系、西岸境界流

The large-scale tropical atmosphere is governed by the weak temperature gradient (WTG) system, in which heating and horizontal divergence are in balance. By contrast, the large-scale midlatitude atmosphere is governed by the quasi-geostrophic (QG) system, in which the Coriolis force and the pressure gradient force are in balance. This difference of atmospheric behaviors are originated from two spatially-variant dimensionless numbers, the Rossby number and the Burger number, both of which depend on the strength of the Earth's rotational effects.

These regions under the WTG and QG systems should be continuously matched at a certain boundary. Therefore, in this study, we aim to theoretically investigate this matching between the WTG and QG solutions at this tropics-midlatitude (TM) boundary. In particular, here we solve a steady-state analytical solution for a smoothly connected QG and WTG systems in a meridional one-dimensional shallow water model on a frictionless f-plane.

In this solution, southerly winds accelerated by heating within the equatorial region are decelerated by radiative cooling in the subtropics. In the midlatitudes, because non-divergent geostrophic winds are dominant, this southerly wind cannot penetrate into the midlatitudes. Therefore, large-scale meridional winds cannot exist at the TM boundary, forming a downward branch of the Hadley circulation. Because the angular momentum originated from the equatorial region cannot be transported into the midlatitudes, a jet stream is generated on the TM boundary. The midlatitude atmospheric state is determined so that the QG solution smoothly matches with the tropical WTG solution, and at the same time, satisfies the boundary condition at the pole. To reproduce the meanderings of the jet stream, the WTG solution near the TM boundary must be further modified by latent heat release from the western boundary currents.