• Clarke, R. A., and J-C. Gascard, 1983: The formation of Labrador Sea Water: Part I: Large-scale processes. J. Phys. Oceanogr., 13 , 17641778.

    • Search Google Scholar
    • Export Citation
  • Coates, M., and G. Ivey, 1997: On convective turbulence and the influence of rotation. Dyn. Atmos. Oceans, 25 , 217232.

  • Coates, M., G. Ivey, and J. Taylor, 1996: Unsteady, turbulent convection into a rotating, linearly stratified fluid: Modeling deep ocean convection. J. Phys. Oceanogr., 26 , 30323051.

    • Search Google Scholar
    • Export Citation
  • D'Asaro, E., D. Farmer, J. Osse, and G. Dairiki, 1996: A Lagrangian float. J. Atmos. Oceanic Technol., 13 , 12301246.

  • Davis, R. E., 1977: Techniques for statistical analysis and prediction of geophysical fluid systems. Geophys. Astrophys. Fluid Dyn., 8 , 245277.

    • Search Google Scholar
    • Export Citation
  • Dickson, R., J. Lazier, J. Meinke, P. Rhines, and J. Swift, 1996: Long-term coordinated changes in the convective activity of the North Atlantic. Progress in Oceanography, Vol. 38, Pergamon, 241–295.

    • Search Google Scholar
    • Export Citation
  • Efron, B., and R. Tibshirani, 1993: An Introduction to the Bootstrap. Chapman and Hall, 436 pp.

  • Fernando, H., R. Chen, and D. Boyer, 1991: Effects of rotation on convective turbulence. J. Fluid Mech., 228 , 513546.

  • Gascard, J., 1991: Open ocean convection and deep water formation revisited in the Mediterranean, Labrador, Greenland, and Weddell Seas. Deep Convection and Deep Water Formation in the Oceans, P. Chu and J. Gascard, Eds., Elsivier, 157–182.

    • Search Google Scholar
    • Export Citation
  • Gascard, J., and R. A. Clarke, 1983: The formation of Labrador Sea water. Part II: Mesoscale and smaller-scale processes. J. Phys. Oceanogr., 13 , 17791797.

    • Search Google Scholar
    • Export Citation
  • Haine, T., and J. Marshall, 1998: Gravitational, symmetric, and baroclinic instability of the ocean mixed layer. J. Phys. Oceanogr., 28 , 634658.

    • Search Google Scholar
    • Export Citation
  • Harcourt, R. R., E. L. Steffen, R. W. Garwood, and E. A. D'Asaro, 2002: Fully Lagrangian floats in Labrador Sea deep convection: Comparison of numerical and experimental results. J. Phys. Oceanogr., 32 , 493510.

    • Search Google Scholar
    • Export Citation
  • Jones, H., and J. Marshall, 1993: Convection with rotation in neutral ocean: A study of open-ocean deep convection. J. Phys. Oceanogr., 23 , 10091039.

    • Search Google Scholar
    • Export Citation
  • Killworth, P., 1983: Deep convection in the world ocean. Rev. Geophys. Space Phys., 21 , 126.

  • Lab Sea Group, 1998: The Labrador Sea Deep Convection Experiment. Bull. Amer. Meteor. Soc., 79 , 20332058.

  • Legg, S., H. Jones, and M. Visbeck, 1996: A heton perspective of baroclinic eddy transfer in localized open ocean convection. J. Phys. Oceanogr., 26 , 22512266.

    • Search Google Scholar
    • Export Citation
  • Legg, S., J. McWilliams, and J. Gao, . 1998: Localization of deep convection by a mesoscale eddy. J. Phys. Oceanogr., 28 , 944970.

  • Lilly, J. M., P. B. Rhines, M. Visbeck, R. Davis, J. R. N. Lazier, F. Schott, and D. Farmer, 1999: Observing deep convection in the Labrador Sea during winter 1994/95. J. Phys. Oceanogr., 29 , 20652098.

    • Search Google Scholar
    • Export Citation
  • Lilly, J. M., P. B. Rhines, M. Visbeck, R. Davis, J. R. N. Lazier, F. Schott, F. Schott, J. Lazier, C. Martens, and E. D'Asaro, . 2001: The structure and variability of the Labrador Sea eddy field, 1994–99. Part I: The mooring perspective. J. Phys. Oceanogr., submitted.

    • Search Google Scholar
    • Export Citation
  • Marshall, J., and F. Schott, 1999: Open-ocean convection: Observations, theory and models. Rev. Geophys., 37 , 164.

  • Maxworthy, T., and S. Narimousa, 1994: Unsteady, turbulent convection into a homogeneous, rotating fluid, with oceanographic application. J. Phys. Oceanogr., 24 , 865887.

    • Search Google Scholar
    • Export Citation
  • Moore, G., K. Alverson, and Z. Hui, 2001: Spatial and temporal variability in the heat and freshwater fluxes associated with the passage of a cyclone over the Labrador Sea. J. Geophys. Res., in press.

    • Search Google Scholar
    • Export Citation
  • Pickart, R., P. Guest, F. Dobson, R. Anderson, K. Bumke, K. Uhlig, U. Karger, and H. Berndt, 1997: Knorr 147 Leg V cruise summary: Labrador Sea convection experiment. Woods Hole Oceanographic Institution Rep., 27 pp.

    • Search Google Scholar
    • Export Citation
  • Prater, M., J. Fontaine, and T. Rossby, 1999: Profiling RAFOS floats in the Labrador Sea: A data report. University of Rhode Island School of Oceanography Tech. Rep. 99-2, 36 pp.

    • Search Google Scholar
    • Export Citation
  • Renfrew, I. A., G. W. K. Moore, P. S. Guest, and K. Bumke, 2002: A comparison of surface layer and surface turbulent flux observations over the Labrador Sea with ECMWF analyses and NCEP reanalyses. J. Phys. Oceanogr., 32 , 383400.

    • Search Google Scholar
    • Export Citation
  • Rossby, T., D. Dorson, and J. Fontaine, 1986: The RAFOS system. J. Atmos. Oceanic Technol., 3 , 672679.

  • Schott, F., M. Visbeck, and U. Send, 1993: Open ocean deep convection, Mediterranean, and Greenland Seas. Ocean Processes on Climate Dynamics: Global and Mediterranean Examples, P. Malanotte-Rizzoli and A. Robinson, Eds., Kluwer Academic, 203–225.

    • Search Google Scholar
    • Export Citation
  • Smith, S., and F. Dobson, 1984: The heat budget at ocean weather ship BRAVO. Atmos.–Ocean, 22 , 115.

  • Straneo, F., and M. Kawase, 1999: Comparisons of localized convection due to localized forcing and preconditioning. J. Phys. Oceanogr., 29 , 5568.

    • Search Google Scholar
    • Export Citation
  • Visbeck, M., J. Marshall, and H. Jones, 1996: Dynamics of isolated convective regions in the oceans. J. Phys. Oceanogr., 26 , 17211734.

    • Search Google Scholar
    • Export Citation
All Time Past Year Past 30 Days
Abstract Views 0 0 0
Full Text Views 310 65 5
PDF Downloads 155 40 3

Deep Convection in the Labrador Sea as Observed by Lagrangian Floats

Elizabeth L. SteffenApplied Physics Laboratory and School of Oceanography, University of Washington, Seattle, Washington

Search for other papers by Elizabeth L. Steffen in
Current site
Google Scholar
PubMed
Close
and
Eric A. D'AsaroApplied Physics Laboratory and School of Oceanography, University of Washington, Seattle, Washington

Search for other papers by Eric A. D'Asaro in
Current site
Google Scholar
PubMed
Close
Restricted access

Abstract

During the winters of 1997 and 1998, a total of 24 Lagrangian floats were deployed in the Labrador Sea. These floats were designed to match the buoyancy and compressibility of seawater. They measured temperature and three-dimensional position (pressure for vertical position and RAFOS acoustic tracking for latitude and longitude) as they followed water motions three-dimensionally. This data provides direct observation of mixed layer depth and excellent estimates of vertical velocity. Floats were repeatedly carried across the convecting layer by vertical velocities averaging several centimeters per second with vertical excursions of up to one kilometer. In the horizontal, several scales of eddy motion were resolved, as was a possible float predilection toward remaining in water preconditioned for convection. Heat flux estimates from this data reveal entrainment and surface heat fluxes similar in magnitude. The mixed layer acts as a vertical conveyor belt of temperature, transporting heat from depth to the surface without requiring a net change in mixed layer temperature, since incorporation of salt from below allows an increase in density without a net change in temperature. Comparison with NCEP reanalysis meteorological heat flux and wind magnitude data shows that the vertical velocity variance can be modeled with 80% skill as a linear function of lagged buoyancy flux (with the atmosphere leading the ocean by ∼1/2 day) without using the wind estimates. Mixed layer motions are clearly driven by the surface buoyancy flux, Bo. A nonrotating scaling of vertical velocity variance, (BoH)1/3, provides a marginally better fit than a rotating scaling, (Bo/f)1/2. Horizontal effects appear to play only a weak role during strong convection but result in rapid restratification when convective forcing weakens.

Corresponding author address: Dr. Elizabeth L. Steffen, Applied Physics Laboratory, University of Washington, 1013 N.E. 40th St., Seattle, WA 98105. Email: steffen@apl.washington.edu

Abstract

During the winters of 1997 and 1998, a total of 24 Lagrangian floats were deployed in the Labrador Sea. These floats were designed to match the buoyancy and compressibility of seawater. They measured temperature and three-dimensional position (pressure for vertical position and RAFOS acoustic tracking for latitude and longitude) as they followed water motions three-dimensionally. This data provides direct observation of mixed layer depth and excellent estimates of vertical velocity. Floats were repeatedly carried across the convecting layer by vertical velocities averaging several centimeters per second with vertical excursions of up to one kilometer. In the horizontal, several scales of eddy motion were resolved, as was a possible float predilection toward remaining in water preconditioned for convection. Heat flux estimates from this data reveal entrainment and surface heat fluxes similar in magnitude. The mixed layer acts as a vertical conveyor belt of temperature, transporting heat from depth to the surface without requiring a net change in mixed layer temperature, since incorporation of salt from below allows an increase in density without a net change in temperature. Comparison with NCEP reanalysis meteorological heat flux and wind magnitude data shows that the vertical velocity variance can be modeled with 80% skill as a linear function of lagged buoyancy flux (with the atmosphere leading the ocean by ∼1/2 day) without using the wind estimates. Mixed layer motions are clearly driven by the surface buoyancy flux, Bo. A nonrotating scaling of vertical velocity variance, (BoH)1/3, provides a marginally better fit than a rotating scaling, (Bo/f)1/2. Horizontal effects appear to play only a weak role during strong convection but result in rapid restratification when convective forcing weakens.

Corresponding author address: Dr. Elizabeth L. Steffen, Applied Physics Laboratory, University of Washington, 1013 N.E. 40th St., Seattle, WA 98105. Email: steffen@apl.washington.edu

Save