日本地球惑星科学連合2019年大会

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[J] 口頭発表

セッション記号 A (大気水圏科学) » A-OS 海洋科学・海洋環境

[A-OS19] 海洋と大気の波動・渦・循環力学

2019年5月27日(月) 10:45 〜 12:15 301A (3F)

コンビーナ:田中 祐希(東京大学大学院理学系研究科)、古恵 亮(APL/JAMSTEC)、久木 幸治(琉球大学)、杉本 憲彦(慶應義塾大学 法学部 日吉物理学教室)、座長:久木 幸治(琉球大学理学部)、相木 秀則

11:00 〜 11:15

[AOS19-08] 赤道太平洋における熱帯不安定波の発生機構

*田中 祐希1日比谷 紀之1 (1.東京大学大学院理学系研究科)

キーワード:熱帯不安定波、赤道太平洋、渦位勾配、ロスビー波、1.5層浅水モデル、線形安定性解析

Tropical instability waves (TIWs) are prominent features observed in the eastern to central equatorial Pacific, which typically have a wavelength of ~1000 km and a period of ~25 days, propagating westward at a speed of ~0.5 m/s. Although TIWs are thought to be generated by meridional shear between the westward-flowing South Equatorial Current (SEC) and the eastward-flowing North Equatorial Countercurrent (NECC), the decisive parameter responsible for the occurrence of the instability has not yet been fully understood. Because the meridional and vertical momentum and heat transfer by TIWs are essential to drive the equatorial ocean circulation and affect the air-sea interactions related to the global climate, a better understanding of the generation mechanism of the TIWs is prerequisite for improving models' capability to predict climate variations.

In this study, we show that a linear stability analysis using a 1.5-layer shallow water model with a zonal mean flow on the equatorial beta plane can successfully predict an unstable mode whose phase speed and meridional structure are both very similar to those of the TIWs simulated in an eddy-resolving ocean general circulation model (OGCM), although the wavelength and the growth rate are somewhat larger and smaller, respectively. This unstable mode can be interpreted as resulting from a coupling between a Rossby wave propagating eastward in the negative potential vorticity (PV) gradient just north of the equator (~1o–3.5oN) while advected westward by the SEC, and a Rossby wave propagating westward in the positive PV gradient further north (~3.5o–8oN) while weakly advected eastward by the NECC. The unstable mode tends to have smaller growth rate as the negative PV gradient becomes weaker, and even disappears when it is completely absent.

The negative PV gradient just north of the equator thus plays an essential role in forming the unstable mode. Actually, the seasonal and interannual variability of the TIWs simulated in the OGCM is shown to be significantly controlled by the strength of the negative PV gradient, suggesting the possibility that it can serve as a key parameter for a dynamically based parameterization of the heat and momentum transfer associated with TIWs in coarse-resolution OGCMs.