Observations of the Labrador Sea eddy field

This paper is an observational study of small-scale coherent eddies in the Labrador Sea, a region of dense water formation thought to be of considerable importance to the North Atlantic overturning circulation. Numerical studies of deep convection emphasize coherent eddies as a mechanism for the lateral transport of heat, yet their small size has hindered observational progress. A large part of this paper is therefore devoted to developing new methods for identifying and describing coherent eddies in two observational platforms, current meter moorings and satellite altimetry. Details of the current and water mass structure of individual eddy events, as they are swept past by an advecting flow, can then be extracted from the mooring data. A transition is seen during mid-1997, with long-lived boundary current eddies dominating the central Labrador Sea year-round after this time, and convectively formed eddies similar to those seen in deep convection modeling studies apparent prior to this time. The TOPEX / Poseidon altimeter covers the Labrador Sea with a loose “net” of observations, through which coherent eddies can seem to appear and disappear. By concentrating on locating and describing anomalous events in individual altimeter tracks, a portrait of the spatial and temporal variability of the underlying eddy field can be constructed. The altimeter results reveal an annual “pulsation” of energy and of coherent eddies originating during the late fall at a particular location in the boundary current, pinpointing the time and place of the boundary current-type eddy formation. The interannual variability seen at the mooring is reproduced, but the mooring site is found to be within a localized region of greatly enhanced eddy activity. Notably lacking in both the annual cycle and interannual variability is a clear relationship between the eddies or eddy energy and the intensity of wintertime cooling. These eddy observations, as well as hydrographic evidence, suggest an active role for boundary current dynamics in shaping the energetics and water mass properties of the interior region.

[1]  J. Lam,et al.  On the beta-drift of an initially circular vortex patch , 2001, Journal of Fluid Mechanics.

[2]  J. Lazier Oceanographic conditions at Ocean Weather Ship Bravo, 1964–1974 , 1980 .

[3]  Frank L. Vernon,et al.  Multitaper spectral analysis of high-frequency seismograms , 1987 .

[4]  S. Häkkinen Decadal Air-Sea Interaction in the North Atlantic Based on Observations and Modeling Results , 2000 .

[5]  K. Heywood,et al.  Seasonal and interannual changes in the North Atlantic subpolar gyre from Geosat and TOPEX/POSEIDON altimetry , 1995 .

[6]  R. Clarke,et al.  Hydrography of the Labrador Sea during Active Convection , 2002 .

[7]  Paul C. Liu,et al.  Wavelet Transforms and Ocean Current Data Analysis , 1996 .

[8]  J. Paduan,et al.  Variability of the near‐surface eddy kinetic energy in the California Current based on altimetric, drifter, and moored current data , 1998 .

[9]  Laurent Labeyrie,et al.  Changes in east Atlantic deepwater circulation over the last 30 , 1994 .

[10]  R. Williamson,et al.  NASA Ocean Altimeter Pathfinder Project. Report 1; Data Processing Handbook , 1998 .

[11]  K. Bumke,et al.  Measurements of Turbulent Fluxes of Momentum and Sensible Heat over the Labrador Sea , 2002 .

[12]  Robert R. Dickson,et al.  Long-term coordinated changes in the convective activity of the North Atlantic , 1996 .

[13]  S. Häkkinen A Simulation of Thermohaline Effects of a Great Salinity Anomaly , 1999 .

[14]  C. Mooers A technique for the cross spectrum analysis of pairs of complex-valued time series, with emphasis on properties of polarized components and rotational invariants , 1973 .

[15]  Stefan Rahmstorf,et al.  Long-Term Global Warming Scenarios Computed with an Efficient Coupled Climate Model , 1999 .

[16]  A. Gordon,et al.  Agulhas Eddies: A Synoptic View Using Geosat ERM Data , 1995 .

[17]  W. Dewar Convection in Small Basins , 2002 .

[18]  B. Tang,et al.  Geostrophic turbulence and emergence of eddies beyond the radius of deformation , 1990 .

[19]  Michael E. Mann,et al.  Interannual Temperature Events and Shifts in Global Temperature: A ''Multiwavelet'' Correlation Approach , 2000 .

[20]  Russ E. Davis,et al.  Observations of Open-Ocean Deep Convection in the Labrador Sea from Subsurface Floats* , 2002 .

[21]  B. Ruddick Intrusive Mixing in a Mediterranean Salt Lens—Intrusion Slopes and Dynamical Mechanisms , 1992 .

[22]  John Marshall,et al.  Convection with Rotation in a Neutral Ocean: A Study of Open-Ocean Deep Convection , 1993 .

[23]  S. Lehman,et al.  Sudden changes in North Atlantic circulation during the last deglaciation , 1992, Nature.

[24]  Detlef Stammer,et al.  Mesoscale Variability in the Atlantic Ocean from Geosat Altimetry and WOCE High-Resolution Numerical Modeling , 1992 .

[25]  L. Talley,et al.  Distribution and Circulation of Labrador Sea Water , 1982 .

[26]  Eric A. D'Asaro,et al.  Structure of two hydrothermal megaplumes , 1994 .

[27]  Robert Hallberg,et al.  Buoyancy-Driven Circulation in an Ocean Basin with Isopycnals Intersecting the Sloping Boundary , 1996 .

[28]  Hans-Harald Hinrichsen,et al.  Can meddies be detected by satellite altimetry , 1991 .

[29]  W. Dewar,et al.  Alignment of lenses: laboratory and numerical experiments , 1994 .

[30]  G. Sutyrin Effects of topography on the beta-drift of a baroclinic vortex , 2001 .

[31]  J. Gascard Mediterranean deep-water formation baroclinic instability and oceanic eddies , 1978 .

[32]  A. Weaver,et al.  Absence of deep-water formation in the Labrador Sea during the last interglacial period , 2001, Nature.

[33]  R. Davis,et al.  Mid-depth recirculation observed in the interior Labrador and Irminger seas by direct velocity measurements , 2000, Nature.

[34]  R. Ray,et al.  NASA Ocean Altimeter Pathfinder Project. Report 2; Data Set Validation , 1999 .

[35]  M. Kawase,et al.  Comparisons of Localized Convection due to Localized Forcing and to Preconditioning , 1999 .

[36]  Carl Wunsch,et al.  Temporal changes in eddy energy of the oceans , 1999 .

[37]  R. Harcourt Numerical simulation of deep convection and the response of drifters in the Labrador Sea , 1999 .

[38]  Lorie K. Bear,et al.  Multi-wavelet analysis of three-component seismic arrays: Application to measure effective anisotropy at Piñon Flats, California , 1999, Bulletin of the Seismological Society of America.

[39]  R. Käse,et al.  Parameterization of Processes in Deep Convection Regimes , 1998 .

[40]  John Marshall,et al.  Restratification after Deep Convection , 1997 .

[41]  U. Schauer A deep saline cyclonic eddy in the west european basin , 1989 .

[42]  P. Rhines,et al.  Convection and restratification in the Labrador Sea, 1990-2000 , 2002 .

[43]  C. Nilsson,et al.  The formation and evolution of East Australian current warm-core eddies , 1980 .

[44]  R. Pingree,et al.  Structure of a meddy (Bobby 92) southeast of the Azores , 1993 .

[45]  R. Clarke,et al.  The Formation of Labrador Sea Water. Part II. Mesoscale and Smaller-Scale Processes , 1983 .

[46]  M. N. Hill,et al.  The sea: ideas and observations on progress in the study of the seas , 1963 .

[47]  M. Visbeck,et al.  Rates and Mechanisms of Water Mass Transformation in the Labrador Sea as Inferred from Tracer Observations , 2002 .

[48]  R. Curry,et al.  Oceanic transport of subpolar climate signals to mid-depth subtropical waters , 1998, Nature.

[49]  S. Rahmstorf,et al.  Sensitivity of Ventilation Rates and Radiocarbon Uptake to Subgrid-Scale Mixing in Ocean Models , 1999 .

[50]  M. Prater,et al.  A Meddy off Cape St. Vincent. Part I: Description , 1994 .

[51]  D. Thomson,et al.  Spectrum estimation and harmonic analysis , 1982, Proceedings of the IEEE.

[52]  J. McWilliams,et al.  Localization of Deep Ocean Convection by a Mesoscale Eddy , 1998 .

[53]  M. Prater Eddies in the Labrador Sea as Observed by Profiling RAFOS Floats and Remote Sensing , 2002 .

[54]  Russ E. Davis,et al.  Observing Deep Convection in the Labrador Sea during Winter 1994/95 , 1999 .

[55]  D. Marshall,et al.  Dynamics of the Mediterranean Salinity Tongue , 1999 .

[56]  S. Rahmstorf On the freshwater forcing and transport of the Atlantic thermohaline circulation , 1996 .

[57]  James C. McWilliams,et al.  Submesoscale, coherent vortices in the ocean , 1985 .

[58]  Dale B. Haidvogel,et al.  A semi-spectral primitive equation ocean circulation model using vertical sigma and orthogonal curvilinear horizontal coordinates , 1991 .

[59]  Jonathan M. Lilly,et al.  Multiwavelet spectral and polarization analyses of seismic records , 1995 .

[60]  W. Zenk,et al.  Large Lenses of Highly Saline Mediterranean Water , 1984 .

[61]  C. Eden,et al.  Sources of Eddy Kinetic Energy in the Labrador Sea , 2002 .

[62]  G. M. Reznik,et al.  The dynamics of baroclinic and barotropic solitary eddies , 1980 .

[63]  H. Rossby,et al.  Mediterranean Water: An Intense Mesoscale Eddy off the Bahamas , 1978, Science.

[64]  E. Boyle,et al.  Deglacial meltwater discharge, North Atlantic Deep Circulation, and abrupt climate change , 1991 .

[65]  P. Guest,et al.  A comparison of surface layer and surface turbulent flux observations over the Labrador Sea with ECMWF analyses and NCEP reanalyses , 2000 .

[66]  Jonathan M. Lilly,et al.  Coherent Eddies in the Labrador Sea Observed from a Mooring , 2002 .

[67]  T. Yamagata,et al.  On the Evolution of Nonlinear Planetary Eddies Larger than the Radius of Deformation , 1982 .

[68]  T. B. Sanford,et al.  The Subthermocline Lens D1. Part I: Description of Water Properties and Velocity Profiles , 1986 .

[69]  John Marshall,et al.  Open‐ocean convection: Observations, theory, and models , 1999 .

[70]  T. Maxworthy,et al.  Unsteady, Turbulent Convection into a Homogeneous, Rotating Fluid,with Oceanographic Applications , 1994 .

[71]  J. McWilliams,et al.  Convective Modifications of a Geostrophic Eddy Field , 2001 .

[72]  E. D’Asaro,et al.  Deep Convection in the Labrador Sea as Observed by Lagrangian Floats , 2002 .

[73]  Russ E. Davis,et al.  The Labrador Sea Deep Convection Experiment , 1998 .

[74]  Philip L. Richardson,et al.  Two Years in the Life of a Mediterranean Salt Lens , 1989 .

[75]  J. Marshall,et al.  Integral Effects of Deep Convection , 1995 .

[76]  E. J. Christensen,et al.  TOPEX/POSEIDON mission overview , 1994 .

[77]  Michael Schröder,et al.  Tracking three meddies with SOFAR floats , 1989 .

[78]  Seelye Martin An introduction to ocean remote sensing , 2004 .

[79]  J. Imberger Physical processes in lakes and oceans , 1998 .

[80]  D. Nof On the β-Induced Movement of Isolated Baroclinic Eddies , 1981 .

[81]  S. Bacon,et al.  Labrador Sea Boundary Currents and the Fate of the Irminger Sea Water , 2002 .

[82]  Ronald B. Smith A hurricane beta-drift law , 1993 .

[83]  M. Farge Wavelet Transforms and their Applications to Turbulence , 1992 .

[84]  S. Legg,et al.  A heton model of the spreading phase of open-ocean deep convection , 1993 .

[85]  L. Polvani,et al.  The emergence of jets and vortices in freely evolving, shallow-water turbulence on a sphere , 1996 .

[86]  R. Clarke,et al.  The Formation of Labrador Sea Water. Part I: Large-Scale Processes , 1983 .

[87]  D. Slepian Prolate spheroidal wave functions, fourier analysis, and uncertainty — V: the discrete case , 1978, The Bell System Technical Journal.

[88]  J. Hesthaven,et al.  Dynamical properties of vortical structures on the beta-plane , 1994, Journal of Fluid Mechanics.

[89]  R. Dickson,et al.  The great salinity anomaly in the northern North Atlantic 1968-1982 , 1988 .

[90]  T. Yamagata,et al.  Asymmetric evolution of eddies in rotating shallow water. , 1994, Chaos.

[91]  Peter D. Killworth,et al.  On the Stability of Oceanic Rings , 1995 .

[92]  Stephen C. Riser,et al.  The Structure, Dynamics, and Origin of a Small-Scale Lens of Water in the Western North Atlantic Thermocline , 1986 .

[93]  D. Hebert,et al.  Evolution of a Mediterranean Salt Lens: Scalar Properties , 1990 .

[94]  James C. McWilliams,et al.  The emergence of isolated coherent vortices in turbulent flow , 1984, Journal of Fluid Mechanics.

[95]  Joseph Gonella,et al.  A rotary-component method for analysing meteorological and oceanographic vector time series , 1972 .

[96]  S. Mallat A wavelet tour of signal processing , 1998 .

[97]  Donald B. Percival,et al.  Spectral Analysis for Physical Applications , 1993 .

[98]  J. LaCasce A Geostrophic Vortex over a Slope , 1998 .