Ocean Turbulence. Part I: One-Point Closure Model—Momentum and Heat Vertical Diffusivities
Top Cited Papers
Open Access
- 1 June 2001
- journal article
- Published by American Meteorological Society in Journal of Physical Oceanography
- Vol. 31 (6) , 1413-1426
- https://doi.org/10.1175/1520-0485(2001)031<1413:otpiop>2.0.co;2
Abstract
Ocean mixing processes have traditionally been formulated using one-point turbulence closure models, specifically the Mellor and Yamada (MY) models, which were pioneered in geophysics using 1980 state-of-the-art turbulence modeling. These models have been widely applied over the years, but the underlying core physical assumptions have hardly improved since the 1980s; yet, in the meantime, turbulence modeling has made sufficient progress to allow four improvements to be made. 1) The value of Ricr. MY-type models yield a low value for the critical Richardson number, Ricr = 0.2 (the result of linear stability is Ricr = 1/4). On the other hand, nonlinear stability analysis, laboratory measurements, direct numerical simulation, large eddy simulation, and mixed layer studies indicate that Ricr ∼ 1. The authors show that by improving the closure for the pressure correlations, the result Ricr ∼ 1 naturally follows. 2) Nonlocal, third-order moments (TOMs). The downgradient approximation used in all models... Abstract Ocean mixing processes have traditionally been formulated using one-point turbulence closure models, specifically the Mellor and Yamada (MY) models, which were pioneered in geophysics using 1980 state-of-the-art turbulence modeling. These models have been widely applied over the years, but the underlying core physical assumptions have hardly improved since the 1980s; yet, in the meantime, turbulence modeling has made sufficient progress to allow four improvements to be made. 1) The value of Ricr. MY-type models yield a low value for the critical Richardson number, Ricr = 0.2 (the result of linear stability is Ricr = 1/4). On the other hand, nonlinear stability analysis, laboratory measurements, direct numerical simulation, large eddy simulation, and mixed layer studies indicate that Ricr ∼ 1. The authors show that by improving the closure for the pressure correlations, the result Ricr ∼ 1 naturally follows. 2) Nonlocal, third-order moments (TOMs). The downgradient approximation used in all models...Keywords
This publication has 49 references indexed in Scilit:
- A dynamical model for turbulence. V. The effect of rotationPhysics of Fluids, 1997
- A dynamical model for turbulence. IV. Buoyancy-driven flowsPhysics of Fluids, 1997
- Determination of the Smagorinsky–Lilly constant CSPhysics of Fluids, 1997
- A dynamical model for turbulence. II. Shear-driven flowsPhysics of Fluids, 1996
- On the performance of a mixed‐layer model based on the κ‐ε turbulence closureJournal of Geophysical Research: Oceans, 1995
- Large Eddy simulation of turbulence: A subgrid scale model including shear, vorticity, rotation, and buoyancyThe Astrophysical Journal, 1994
- Variability of the Tropical Atlantic Ocean Simulated by a General Circulation Model with Two Different Mixed-Layer PhysicsJournal of Physical Oceanography, 1993
- Modeling the effects of buoyancy on the evolution of geophysical boundary layersJournal of Geophysical Research: Oceans, 1992
- Turbulent convection with overshooting - Reynolds stress approachThe Astrophysical Journal, 1992
- Richardson Number Criterion for the Nonlinear Stability of Three-Dimensional Stratified FlowPhysical Review Letters, 1984