Abstract

Abstract. Analytical solutions are found for the problem of instability of a weak geostrophic flow with linear velocity shear accounting for vertical diffusion of buoyancy. The analysis is based on the potential-vorticity equation in a long-wave approximation when the horizontal scale of disturbances is considered much larger than the local baroclinic Rossby radius. It is hypothesized that the solutions found can be applied to describe stable and unstable disturbances of the planetary scale with respect, in particular, to the Arctic Ocean, where weak baroclinic fronts with typical temporal variability periods on the order of several years or more have been observed and the β effect is negligible. Stable (decaying with time) solutions describe disturbances that, in contrast to the Rossby waves, can propagate to both the west and east, depending on the sign of the linear shear of geostrophic velocity. The unstable (growing with time) solutions are applied to explain the formation of large-scale intrusions at baroclinic fronts under the stable–stable thermohaline stratification observed in the upper layer of the Polar Deep Water in the Eurasian Basin. The suggested mechanism of formation of intrusions can be considered a possible alternative to the mechanism of interleaving at the baroclinic fronts due to the differential mixing.

Highlights

  • The study of intrusions in oceanic frontal zones is required to understand the mechanism of ventilation and mixing in the ocean interior

  • It can be suggested that the thermohaline intrusions within the upper layer of Polar Deep Water (PDW) are driven by differential mixing

  • We analytically investigated the instability of a baroclinic front in the quasi-geostrophic, long-wave approximation taking into account the vertical diffusion of buoyancy

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Summary

Introduction

The study of intrusions in oceanic frontal zones is required to understand the mechanism of ventilation and mixing in the ocean interior (see, e.g., Zhurbas et al, 1993, 1987; Rudels et al, 1999, 2009; Kuzmina and Zhurbas, 2000; Walsh and Ruddick, 2000; Merryfield, 2000; Radko, 2003; Richards and Edwards, 2003; Kuzmina et al, 2005, 2011; Smyth and Ruddick, 2010). Proceeding from the analogy between the equations describing the dynamics of large-scale atmospheric perturbations and the Orr–Sommerfeld equation (Lin, 1955; Stern, 1975), Miles (1965) analyzed the instability of the critical layer (a very thin layer in which the phase velocity of a disturbance equals the velocity of zonal flow) This resulted in an analytical asymptotic solution accounting for a very small, though finite, vertical diffusion of buoyancy. Taking into account that the influence of the β effect on the dynamics of large-scale disturbances is negligible in the Polar Ocean for near the pole, it seems reasonable to suggest that the contribution of diffusion of buoyancy to the destabilization of weak geostrophic currents can be important In such circumstances one would expect the formation of intrusions, rather than vortices.

Unstable solutions
Stable solutions
Obtained solutions: discussion
Conclusions
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