Pawlowicz Ryszard A.

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Ryszard A.

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  • Thesis
    Tomographic observations of deep convection and the thermal evolution of the Greenland Sea Gyre, 1988-1989
    (Massachusetts Institute of Technology and Woods Hole Oceanographic Institution, 1994-02) Pawlowicz, Ryszard A.
    The thermal evolution of the Greenland Sea Gyre is investigated using both historical data and tomographic results from the 1988-89 Greenland Sea Tomography Experiment. Thermal evolution of the gyre center divides naturally into three periods: a preconditioning phase (November-January), during which surface salinity is increased by brine rejection from ice formation and by entrainment but in which the mixed-layer deepens only slowly to a depth of some 150-200m, a deep mixing phase (February-March) during which the surface mixed-layer deepens rapidly to approximately 1500m in the gyre center purely under the influence of local surface cooling, and a restratification phase during which the products of deep mixing are replaced by inflowing Arctic Intermediate Water (AIW). The onset of the deep mixing phase occurs after ice formation in the gyre center stops, resulting in an area of open water where large heat fluxes can occur. In surrounding regions, including the odden region to the south, ice is still being formed, and the mixed layer does not deepen significantly. To the north and west, closer to the steep topography of the continental shelf, the inverse results show significant variability due to advection, and large temperature and heat content fluctuations with a period of about 50 days are seen. The effects of advection are deduced from heat and salt budgets, and appear to be important only during the restratification phase for intermediate depths, and only during the summer for the surface waters. Comparison of the tomographic results with point measurements indicates that deep mixing occurs in a field of small plumes in which dense water sinks downwards, surrounded by larger regions of upwelling. The plume geometry is consistent with that predicted by numerical and laboratory models. Dynamical processes for bringing the AIW to the surface in order to form deep water are not needed in this scenario, rather the surface waters are modified until they match the density of the AIW after which surface cooling drives convection.