Evidence for slow mixing across the pycnocline from an open-ocean tracer-release experiment

THE distributions of heat, salt and trace substances in the ocean thermocline depend on mixing along and across surfaces of equal density (isopycnal and diapycnal mixing, respectively). Measurements of the invasion of anthropogenic tracers, such as bomb tritium and 3He (see, for example, refs 1 and 2), have indicated that isopycnal processes dominate diapycnal mixing, and turbulence measurements have suggested that diapycnal mixing is small3,4, but it has not been possible to measure accurately the diapycnal diffusivity. Here we report such a measurement, obtained from the vertical dispersal of a patch of the inert compound SF6 released in the open ocean. The diapycnal diffusivity, averaged over hundreds of kilometres and five months, was 0.11 ± 0.02 cm2 s−1, confirming previous estimates1–4. Such a low diffusivity can support only a rather small diapycnal flux of nitrate into the euphotic zone; it justifies the neglect of diapycnal mixing in dynamic models of the thermocline25–27, and implies that heat, salt and tracers must penetrate the thermocline mostly by transport along, rather than across, density surfaces.

[1]  A. Watson,et al.  The Santa Monica Basin tracer experiment: Comparison of release methods and performance of perfluorodecalin and sulfur hexafluoride , 1991 .

[2]  B. Peterson,et al.  Particulate organic matter flux and planktonic new production in the deep ocean , 1979, Nature.

[3]  A. Watson,et al.  The Santa Monica Basin tracer experiment: A study of diapycnal and isopycnal mixing , 1991 .

[4]  P. Welander An Advective Model of the Ocean Thermocline , 1959 .

[5]  J. Moum,et al.  Mixing in the Main Thermocline , 1986 .

[6]  A. Watson,et al.  Analysis of sulfur hexafluoride in seawater , 1991 .

[7]  J. Pedlosky,et al.  The Ventilated Thermocline , 1983 .

[8]  N. S. Oakey,et al.  EPSONDE: an instrument to measure turbulence in the deep ocean , 1988 .

[9]  M. Gregg,et al.  Scaling turbulent dissipation in the thermocline , 1989 .

[10]  W. Jenkins,et al.  Nitrate flux into the euphotic zone near Bermuda , 1988, Nature.

[11]  G. Siedler,et al.  Baroclinic Flow and Transient-Tracer Fields in the Canary–Cape Verde Basin , 1986 .

[12]  D. Haidvogel,et al.  Tracer dispersal by mid-ocean mesoscale eddies. Part I. Ensemble statistics , 1984 .

[13]  C. Garrett On the initial streakness of a dispersing tracer in two- and three-dimensional turbulence , 1983 .

[14]  R. Huang The Three‐Dimensional Structure of Wind‐Driven Gyres: Ventilation and Subduction , 1991 .

[15]  M. Altabet,et al.  Nitrogen transport by vertically migrating diatom mats in the North Pacific Ocean , 1993, Nature.

[16]  A. Watson,et al.  Recent history of atmospheric trace gas concentrations deduced from measurements in the deep sea: Application to sulphur hexafluoride and carbon tetrachloride , 1985 .

[17]  William R. Young,et al.  Shear-Flow Dispersion, Internal Waves and Horizontal Mixing in the Ocean , 1982 .

[18]  H. Stommel,et al.  Four Views of a Portion of the North Atlantic Subtropical Gyre , 1983 .