Abstract

Abstract. This work presents the quantitative study of climatological distributions of mid-depth source water types in the northeast (NE) Atlantic using the optimum multiparameter analysis (OMP). It generalises a number of regional results from particular synoptic sections. The cores of the Mediterranean Water (MW), the modified Antarctic Intermediate Water (mAAIW) and the Subarctic Intermediate Water (SAIW) are detected and spatial variations of their depth/density are obtained: as expected, spreading of the water types is predominantly isopycnic and follows the major mid-depth circulation patterns. In some areas the turbulent transport also makes a considerable contribution. MW in the Atlantic spreads in three cores of different density: the upper MW core (northwest of the line 28° W, 35° N–14° W, 44° N) is found in the neutral density range of 27.65–27.70 kg m−3 at depths of 900–1000 m; the main MW core (between the line above and the line 35° W, 28° N–10° W, 37° N) has neutral density of around 27.75 kg m−3 and is found at 1000–1100 m; the lower MW core (southeast of the line 35° W, 28° N–10° W, 37° N) has neutral density of around 27.80 kg m−3 and is found at 1250–1350 m. The upper MW core has a comparatively low MW content (below 30 %) and is speculated to be transported by the mean flow from the northern Iberian Peninsula and the Bay of Biscay to the northern Azores. The main MW core contains the majority of the outflowing MW. It primarily originates from the Mediterranean undercurrent around Estremadura Promontory, where the Joint Effect of Baroclinicity and Bottom Relief (JEBAR) overrides the topographic β effect. It is transported west to the Azores Islands mostly along 39° N. The lower MW core originates in the Gulf of Cádiz, from where it is transported by the dominating flows southwestwards. The SAIW core is detected between 27.70 and 27.75 kg m−3. It is found to spread south along both slopes of the Mid-Atlantic Ridge (MAR). SAIW east of the MAR mixes with the upper and the main MW cores and re-circulates in a cyclonic gyre at 15–25° W and 34–39° N, penetrating as far south as the Azores Current. The mAAIW core is detected between 27.60 and 27.65 kg m−3. Its northernmost spreading limit is between 25 and 29° N, but its influence can be observed along the African coast and immediately west of the Canary Islands up to 32° N. The maximum concentration of the mAAIW core is found south of the Canary Islands, from where mAAIW is advected westwards, along with the westward spreading of the deep fraction of MW.

Highlights

  • Thermohaline properties of deep oceanic waters are formed in the upper mixed layer under the effects of the solar radiation balance and the heat/fresh water exchanges between the ocean and the atmosphere

  • Results of the optimum multiparameter analysis (OMP) analysis critically depend on the choice of the dominating source water types

  • A significant crossisopycnal deepening of the lower boundary of North Atlantic Central Water (NACW) occurs near the Iberian Peninsula (Fig. 4c)

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Summary

Introduction

Thermohaline properties of deep oceanic waters are formed in the upper mixed layer under the effects of the solar radiation balance and the heat/fresh water exchanges between the ocean and the atmosphere. The deep convection is a result of the gravitational instability and is mostly active in weakly stratified polar waters in winter due to an intensive heat loss and water salinification during ice formation (van Aken, 2000a). When a subduction/convection process is regular, large collections of water parcels with a common formation history form Those are known as the source water types (Tomczak and Large, 1989). The early works only present qualitative descriptions of the distributions of water types, and are mostly based on subjective criteria. Detailed knowledge of the distributions of water types permits a view of the major pathways of water particles across the mid-depth ocean, which is otherwise too slow and turbulent to confidently derive such pathways from the limited number of observations currently available.

Upper water masses
Intermediate water masses
Deep water masses
The data sets
The optimum multiparameter analysis set-up
The accuracy of the OMP analysis
Distribution of source water types in the subtropical NE Atlantic
Advective transport of source water types
Discussion and conclusions
Obtaining gridded Eulerian velocity fields from Argo and RAFOS data sets
Comparison of our results with some previous studies
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