Abstract

The available historical oxygen data show that the deepest part of the South Adriatic Pit remains well-ventilated despite the winter convection reaching only the upper 700 m depth. Here, we show that the evolution of the vertical temperature structure in the deep South Adriatic Pit (dSAP) below the Otranto Strait sill depth (780 m) is described well by continuous diffusion, a continuous forcing by heat fluxes at the upper boundary (Otranto Strait sill depth) and an intermittent forcing by rare (several per decade) deep convective and gravity-current events. The analysis is based on two types of data: (i) 13-year observational data time series (2006–2019) at 750, 900, 1,000, and 1,200 m depths of the temperature from the E2M3A Observatory and (ii) 55 vertical profiles (1985–2019) in the dSAP. The analytical solution of the gravest mode of the heat equation compares well to the temperature profiles, and the numerical integration of the resulting forced heat equation compares favorably to the temporal evolution of the time-series data. The vertical mixing coefficient is obtained with three independent methods. The first is based on a best fit of the long-term evolution by the numerical diffusion-injection model to the 13-year temperature time series in the dSAP. The second is obtained by short-time (daily) turbulent fluctuations and a Prandtl mixing length approximation. The third is based on the zero and first modes of an Empirical Orthogonal Function (EOF) analysis of the time series between 2014 and 2019. All three methods are compared, and a diffusivity of approximately κ = 5 · 10−4m2s−1 is obtained. The eigenmodes of the homogeneous heat equation subject to the present boundary conditions are sine functions. It is shown that the gravest mode typically explains 99.5% of the vertical temperature variability (the first three modes typically explain 99.85%) of the vertical temperature profiles at 1 m resolution. The longest time scale of the dissipative dynamics in the dSAP, associated with the gravest mode, is found to be approximately 5 years. The first mode of the EOF analysis (85%) represents constant heating over the entire depth, and the zero mode is close to the parabolic profile predicted by the heat equation for such forcing. It is shown that the temperature structure is governed by continuous warming at the sill depth and deep convection and gravity current events play less important roles. The simple model presented here allows evaluation of the response of the temperature in the dSAP to different forcings derived from climate change scenarios, as well as feedback on the dynamics in the Adriatic and the Mediterranean Sea.

Highlights

  • The paradigm of the vertical temperature structure of the deep ocean is given by the “Abyssal recipes” of Munk (1966)

  • We performed a numerical integration of the heat equation with an imposed temperature at approximately the sill depth Tobs(−750 m, t) (Dirichlet boundary condition) and a vanishing gradient at the bottom (1,220 m) (Neumann boundary condition)

  • All the above results based on temperature measurements show that the action of turbulent mixing in the deep South Adriatic Pit (dSAP) can be modeled well by a heat equation with a constant diffusion coefficient in space and time, a prescribed heat flux at the sill depth and a forcing term that represents rare gravity current and deep convection events

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Summary

Introduction

The paradigm of the vertical temperature structure of the deep ocean is given by the “Abyssal recipes” of Munk (1966) It is based on a balance between an upward advective cooling and a downward diffusion of heat, which leads to an exponential profile of the temperature in the vertical direction. Mixing in the boundary layers and generation by wind-driven horizontal turbulence are other possible sources of mixing (see Vallis, 2017 for a pedagogical discussion). These considerations can be applied to the Adriatic Sea (see Figure 1), whose dynamics have been widely studied in a large number of publications (see, e.g., the review by Cushman-Roisin et al, 2001). The ventilation should be associated with some other processes, such as vertical diffusion

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