JpGU-AGU Joint Meeting 2017

講演情報

[EE] 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-OS15] [EE] 海洋混合に関わる諸問題

2017年5月21日(日) 13:45 〜 15:15 A09 (東京ベイ幕張ホール)

コンビーナ:日比谷 紀之(東京大学大学院理学系研究科地球惑星科学専攻)、Louis St Laurent(Woods Hole Oceanographic Institution)、Ren-Chieh Lien(None)、Robin Ann Robertson(University of New South Wales Canberra)、座長:Robertson Robin(University of New South Wales Canberra)、座長:日比谷 紀之(東京大学 大学院理学系研究科 地球惑星科学専攻)

15:00 〜 15:15

[AOS15-18] Kinetic Energy Flux Budget Across Air-sea Interface

*Yalin Fan1 (1.Naval Research Laboratory)

キーワード:turbulent kinetic energy, surface gravity waves, high winds

The kinetic energy (KE) fluxes into subsurface currents (EFc) is important boundary condition for vertical mixing in ocean circulation models. Traditionally, numerical models assume the KE flux from wind is identical to the KE flux into subsurface currents, that is, no net KE is gained (or lost) by surface waves. This assumption, however, is invalid when the surface wave field is not fully developed. When the surface wave field grows in space or time, it acquires kinetic energy, hence, reduces the KE fluxes into subsurface currents compared to the fluxes from wind. In this study, numerical experiments are performed to investigate the KE flux budget across the air-sea interface under both uniform and idealized tropical cyclone winds. The wave fields are simulated using the WAVEWATCH III model under various wind forcing. The difference between the KE flux from wind and that into ocean currents is estimated using an air-sea KE budget model. To address the uncertainty of these estimates resides in the variation of source functions, two source function packages are used for this study: the coupled wind wave model by Moon et al (2004) and the ST4 source package by Ardhuin et al (2010). Simulated KE flux into the ocean currents are found to be consistent with field observations by Terray et al. (1996) and Drennan et al (1996). It is significantly reduced relative to the KE flux input from wind under growing seas. The reduction can be as large as 20%, and the variation of this ratio is highly dependent on the choice of source function for the wave model. Our results also suggest that the normalized KE flux by the friction velocity cube (u*^3) may depend on both wave age and friction velocity (u*), and a new parameterization for EFc is proposed.