Subpolar Mode Water in the northeastern Atlantic: 2. Origin and transformation

[1] The processes that lead to the transformation and origin of the eastern North Atlantic Subpolar Mode Waters (SPMW) are investigated from observational data using an extended Walin framework. Air-sea flux data from the National Oceanography Center, Southampton (NOCS), and hydrographic data from the A24 cruise collected during the World Ocean Circulation Experiment (WOCE) are used to estimate the contribution of diapycnal and isopycnal fluxes to the density classes that include SPMW. Surface diapycnal volume flux is the dominant source of waters in the SPMW density. In the North Atlantic subpolar gyre the diapycnal volume flux occurs along the main branches of the North Atlantic Current (NAC) and it has an average transport of 14 ± 6.5 Sv, with a maximum of 21.5 Sv across the 27.35sq isopycnal. The regional distribution of the diapycnal flux on isopycnal surfaces is computed to identify the areas with the largest diapycnal flux. These regions coincide with the location of SPMW based on potential vorticity. The surface diapycnal flux is associated with obduction and subduction through the permanent pycnocline. Therefore, the water involved in the transformation of SPMWs is continuously exchanged with the ocean interior. In addition, we suggest that subduction is not associated with smooth advection from the mixed layer to the ocean interior, but is water mass loss entrainment into the deep overflows of the subpolar gyre. The isopycnal component of the SPMW throughput is estimated from the geostrophic transport across the A24 section from Greenland to Scotland and is 10% to 40% of the diapycnal flux.

[1]  Randy Showstack,et al.  World Ocean Database , 2009 .

[2]  L. Talley,et al.  Subpolar Mode Water in the northeastern Atlantic: 1. Averaged properties and mean circulation , 2008 .

[3]  Timothy P. Boyer,et al.  World ocean database 2009 , 2006 .

[4]  A. Tréguier,et al.  Effects of the Mixed Layer Time Variability on Kinematic Subduction Rate Diagnostics , 2005 .

[5]  Transformation of the Warm Waters of the North Atlantic from a Geostrophic Streamfunction Perspective , 2004 .

[6]  Liuzhi Zhao,et al.  Mixed layer transformation for the North Atlantic for 1990–2000 , 2004 .

[7]  S. Josey,et al.  Inverse Analysis Adjustment of the SOC Air-Sea Flux Climatology Using Ocean Heat Transport Constraints , 2003 .

[8]  J. Molines,et al.  Water Mass Transformation in the North Atlantic and Its Impact on the Meridional Circulation: Insights from an Ocean Model Forced by NCEP–NCAR Reanalysis Surface Fluxes , 2003 .

[9]  K. Speer,et al.  Large-Scale Vertical and Horizontal Circulation in the North Atlantic Ocean , 2003 .

[10]  A. Ganachaud Large-scale mass transports, water mass formation, and diffusivities estimated from World Ocean Circulation Experiment (WOCE) hydrographic data , 2003 .

[11]  L. Talley Shallow, Intermediate, and Deep Overturning Components of the Global Heat Budget , 2003 .

[12]  Fiammetta Straneo,et al.  Is Labrador Sea Water formed in the Irminger basin , 2003 .

[13]  J. Church,et al.  Ocean Circulation and Climate: Observing and Modelling the Global Ocean , 2001 .

[14]  W. Large,et al.  Ocean surface water mass transformation , 2001 .

[15]  C. Mauritzen,et al.  On the origin of the warm inflow to the Nordic Seas , 2001 .

[16]  W. Large,et al.  Chapter 5.1 Ocean surface water mass transformation , 2001 .

[17]  L. Talley,et al.  Chapter 5.4 Mode waters , 2001 .

[18]  R. Marsh Recent Variability of the North Atlantic Thermohaline Circulation Inferred from Surface Heat and Freshwater Fluxes , 2000 .

[19]  J. F. Read,et al.  CONVEX-91: water masses and circulation of the Northeast Atlantic subpolar gyre , 2000 .

[20]  Richard G. Williams,et al.  Diagnosing Water Mass Formation from Air–Sea Fluxes and Surface Mixing , 1999 .

[21]  Johan Nilsson,et al.  Reconciling thermodynamic and dynamic methods of computation of water-mass transformation rates , 1999 .

[22]  K. Speer A note on average cross-isopycnal mixing in the North Atlantic ocean , 1997 .

[23]  C. Garrett,et al.  The effects on water mass formation of surface mixed layer timedependence and entrainment fluxes , 1997 .

[24]  M. Arhan,et al.  Oceanic Ventilation in the Eastern North Atlantic , 1996 .

[25]  P. M. Saunders The Flux of Dense Cold Overflow Water Southeast of Iceland , 1996 .

[26]  B. Qiu,et al.  Ventilation of the North Atlantic and North Pacific: Subduction Versus Obduction , 1995 .

[27]  K. Speer,et al.  Water Mass Formation from Revised COADS Data , 1995 .

[28]  K. Speer,et al.  The Relationship between Water Mass Formation and the Surface Buoyancy Flux, with Application to Phillips’ Red Sea Model , 1995 .

[29]  W. Schmitz On the interbasin‐scale thermohaline circulation , 1995 .

[30]  R. Dickson,et al.  The production of North Atlantic Deep Water: Sources, rates, and pathways , 1994 .

[31]  J. Marshall,et al.  Inferring the Subduction Rate and Period over the North Atlantic , 1993 .

[32]  W. Schmitz,et al.  On the North Atlantic Circulation , 1993 .

[33]  Eli Tziperman,et al.  Rates of Water Mass Formation in the North Atlantic Ocean , 1992 .

[34]  W. Krauss The North Atlantic Current , 1986 .

[35]  Eli Tziperman,et al.  On the Role of Interior Mixing and Air-Sea Fluxes in Determining the Stratification and Circulation of the Oceans , 1986 .

[36]  L. Talley,et al.  Warm-to-Cold Water Conversion in the Northern North Atlantic Ocean , 1984 .

[37]  L. Talley,et al.  The subpolar mode water of the North Atlantic , 1982 .

[38]  Gösta Walin,et al.  On the relation between sea‐surface heat flow and thermal circulation in the ocean , 1982 .

[39]  Jotaro Masuzawa,et al.  Subtropical mode water , 1969 .

[40]  L. V. Worthington,et al.  Deep currents south of iceland , 1962 .