Abstract
In this study, M2 tidal energy and tide-induced mixing in the Mariana double ridges are investigated with a high-resolution three-dimensional non-hydrostatic numerical model and baroclinic energy budget analysis. The interference effect of the double ridges on the internal tide in the Mariana is examined by omitting either the eastern or the western ridge. Our results show that the baroclinic velocity on the sides of the interior facing slopes of the double ridges is larger than that on the other sides. In the double ridges, high values of dissipation reaching O (10−6 W kg−1) are accompanied by diapycnal diffusivity reaching O (10−1 m2 s−1), which is several orders of magnitude higher than the mixing of the open ocean. The bottom diapycnal mixing in the inner region between the two ridges is one order of magnitude larger than the mixing outside the ridges, indicating the important role of the interference of the double-ridge topography on the mixing in the Mariana Arc. Omitting either the eastern or the western ridge would have a significant impact on tide current, baroclinic energy flux and dissipation, and diapycnal mixing. The internal tide conversion, dissipation, and flux divergence are amplified by the double ridge topography, especially in the central part of the double ridges. Through energy budgets analysis, we conclude that the eastern ridge is the main source of the baroclinic tide in the Mariana double ridges.
Highlights
Vertical mixing is ubiquitous in the global ocean
Such a mechanism has been found to be the internal tide breaking, which plays an important role in the enhancement of diapycnal mixing
The dissipation rate is reduced significantly compared with that under the DR case, Comparing the three cases, we find that omitting one ridge has a significant effect on the diapycnal diffusivity
Summary
Vertical mixing is ubiquitous in the global ocean. It determines kinetic energy, heat energy, and material transport in the ocean, and is essential for maintaining ocean stratification and meridional overturning circulation. Munk and Wunsch [2] pointed out that in order to maintain the current strength of the oceanic thermohaline circulation, the average ocean mixing rate must be at least 10−4 m2 s−1 , which means that there must be a strong mixing caused by a special mechanism in the ocean to support the normal thermohaline circulation of the ocean. Such a mechanism has been found to be the internal tide breaking, which plays an important role in the enhancement of diapycnal mixing
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