Japan Geoscience Union Meeting 2023

Presentation information

[J] Oral

A (Atmospheric and Hydrospheric Sciences ) » A-CG Complex & General

[A-CG38] Dynamics of Oceanic and Atmospheric Waves, Vortices, and Circulations

Mon. May 22, 2023 10:45 AM - 12:15 PM 102 (International Conference Hall, Makuhari Messe)

convener:Kunihiro Aoki(Meteorological Research Institute, Japan Meteorological Agency), Satoshi Osafune(Japan Agency for Marine-Earth Science and Technology), Yukiharu Hisaki(University of the Ryukyus), Norihiko Sugimoto(Keio University, Department of Physics), Chairperson:Kunihiro Aoki(Japan Meteorological Agency), Satoshi Osafune(Japan Agency for Marine-Earth Science and Technology), Yukiharu Hisaki(University of the Ryukyus), Norihiko Sugimoto(Keio University, Department of Physics)

12:00 PM - 12:15 PM

[ACG38-06] Numerical Simulation of Upper Ocean Responses to the Passage of a Submesoscale Eddy

*Yalin Fan1 (1.U.S. Naval Research Laboratory)

Keywords:boundary layer turbulence, submesoscale dynamics, turbulence simulation

In this study, a large eddy simulation model (LES) is used to investigate the effect of an idealized submesoscale eddy on ocean surface boundary layer turbulence. Large scale forcing (LSF) terms are introduced to the model to represent the effects of submesocale eddies using the scale separation approach.

Although re-stratification is observed at the arrival of the eddy center, consistent with previous studies, strong mixing and deepening is detected before/after the arrival of the eddy center. LES experiments are conducted to investigate the mechanism behind these dynamical responses, and explore the relative importance of the LSF terms. The interaction among these forcing terms is shown to be highly nonlinear, and the combined effects of buoyancy and momentum eddy forcing dominate the boundary layer response to the submesoscale eddy. While buoyancy flux is responsible for the enhanced mixing in the boundary layer, our analysis suggests that the momentum eddy forcing can significantly alter the timing of the enhanced mixing and boost its strength through generating strong mean current in the water column that accelerates westward density advection generated by the buoyancy eddy forcing. The lighter/heavier fluid intrusion brought by the mean flow leads to strong upwelling/downwelling, enhanced mixing and deepening of the mixed layer before the arrival of the eddy.

Eddy distortion due to its asymmetric decay with time and northward Ekman transport generated by the wind stress also leads to substantial differences in boundary layer responses at different locations relative to the eddy center.