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On the behaviour of the residence time at the bottom of the mixed layer
Authors:Eric Deleersnijder  Jean-Marie Beckers  Eric J M Delhez
Institution:1. G. Lema?tre institute of astronomy and geophysics (ASTR) and Centre for systems engineering and applied mechanics (CESAME), Université catholique de Louvain, 4 Avenue G. Lema?tre, 1348, Louvain-la-Neuve, Belgium
2. Océanographie Physique, Département d′Astrophysique, Géophysique et Océanographie (AGO), Université de Liège, Sart Tilman B5, 17 Allée du 6 Ao?t, 4000, Liège, Belgium
3. Modélisation et Méthodes Mathématiques, Département d′Aérospatiale et Mécanique, Université de Liège, Sart Tilman B37, 12 Grande Traverse, 4000, Liège, Belgium
Abstract:To understand why the findings of Deleersnijder et al. (2006), Environ Fluid Mech 6: 25–42]—the residence time in the mixed layer in not necessarily zero at the pycnocline—are consistent with those of Delhez and Deleersnijder (2006), Ocean Dyn 56:139–150]—the residence time in a control domain vanishes at the open boundaries of this control domain—, it is necessary to consider a control domain that includes part of the pycnocline, in which the eddy diffusivity is assumed to be zero. Then, depending on the behaviour of the eddy diffusivity near the bottom of the mixed layer, the residence time may be seen to exhibit a discontinuity at the interface between the mixed layer and the pycnocline. If such a discontinuity exists, the residence time is non-zero in the former and zero in the latter. This is illustrated by analytical solutions obtained under the assumption that the eddy diffusivity is constant in the mixed layer.
Keywords:Adjoint model  Mixed mayer  Pycnocline  Residence time
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