Analysis of STCC eddies using the Okubo–Weiss parameter on model and satellite data

The North Pacific Subtropical Counter Current (STCC) is a weak zonal current comprising of a weak eastward flow near the surface (with speeds of less than 0.1 m/s and a thickness of approximately 50–100 m) and westward flow (the North Equatorial Current) beneath. Previous studies (e.g., Qiu J Phys Oceanogr 29: 2471–2486, 1999) have shown that the STCC is baroclinically unstable. Therefore, despite its weak mean speeds, nonlinear STCC eddies with diameters ~300 km or larger and rotational speeds exceeding the eddy propagation speeds develop (Samelson J Phys Oceanogr 27: 2645–2662, 1997; Chelton et al. Prog Oceanogr 91: 167–216, 2011). In this study, the authors present numerical experiments to describe and explain the instability and eddy-generation processes of the STCC and the seasonal variation. Emphasis is on finite-amplitude eddies which are analyzed based on the parameter of Okubo (Deep-Sea Res 17: 445–454, 1970) and Weiss (Physica D 48: 273–294, 1991). The temperature and salinity distribution in March and April offer the favorable condition for eddies to grow, while September and October are unfavorable seasons for the generation of eddies. STCC is maintained not only by subsurface front but also by the sea surface temperature (SST) front. The seasonal variation of the vertical shear is dominated by the seasonal surface STCC velocity. The SST front enhances the instability and lead to the faster growth of STCC eddies in winter and spring. The near-surface processes are therefore crucial for the STCC system.

[1]  T. Yamagata,et al.  Roles of Mesoscale Eddies in the Kuroshio Paths , 2004 .

[2]  R. Samelson Coastal Boundary Conditions and the Baroclinic Structure of Wind-Driven Continental Shelf Currents* , 1997 .

[3]  D. Chelton,et al.  Global observations of nonlinear mesoscale eddies , 2011 .

[4]  S. Xie,et al.  Interannual variability of the North Pacific Subtropical Countercurrent: role of local ocean–atmosphere interaction , 2012, Journal of Oceanography.

[5]  Yu-Lin Chang,et al.  The Philippines–Taiwan Oscillation: Monsoonlike Interannual Oscillation of the Subtropical–Tropical Western North Pacific Wind System and Its Impact on the Ocean , 2012 .

[6]  Yu-Lin Chang,et al.  Instability of the North Pacific subtropical countercurrent , 2014 .

[7]  L. Oey,et al.  Blocking and Westward Passage of Eddies in the Luzon Strait , 2010 .

[8]  P. Lin,et al.  Mesoscale eddies in the northwestern subtropical Pacific Ocean: Statistical characteristics and three-dimensional structures , 2013 .

[9]  N. Heaps,et al.  Three-dimensional coastal ocean models , 1987 .

[10]  L. Oey,et al.  Interannual and seasonal variations of Kuroshio transport east of Taiwan inferred from 29 years of tide‐gauge data , 2011 .

[11]  K. Hanawa,et al.  Subsurface Subtropical Fronts of the North Pacific as Inherent Boundaries in the Ventilated Thermocline , 2002 .

[12]  B. Qiu,et al.  Seasonal variation of eddy kinetic energy of the North Pacific Subtropical Countercurrent simulated by an eddy‐resolving OGCM , 2007 .

[13]  Yu-Lin Chang,et al.  ATOP -The advanced Taiwan ocean prediction system based on the mpiPOM. Part 1: Model descriptions, analyses and results , 2013 .

[14]  Tal Ezer,et al.  Loop Current warming by Hurricane Wilma , 2006 .

[15]  J. Weiss The dynamics of entropy transfer in two-dimensional hydrodynamics , 1991 .

[16]  Caskey,et al.  GENERAL CIRCULATION EXPERIMENTS WITH THE PRIMITIVE EQUATIONS I . THE BASIC EXPERIMENT , 1962 .

[17]  M. Uda,et al.  The eastward subtropical countercurrent in the western North Pacific Ocean , 1969 .

[18]  J. Smagorinsky,et al.  GENERAL CIRCULATION EXPERIMENTS WITH THE PRIMITIVE EQUATIONS , 1963 .

[19]  A. Ōkubo Horizontal dispersion of floatable particles in the vicinity of velocity singularities such as convergences , 1970 .

[20]  A. Blumberg,et al.  A Description of a Three‐Dimensional Coastal Ocean Circulation Model , 2013 .

[21]  A. Watson,et al.  Bio‐optical feedbacks among phytoplankton, upper ocean physics and sea‐ice in a global model , 2005 .

[22]  Antoni Jordi,et al.  sbPOM: A parallel implementation of Princenton Ocean Model , 2012, Environ. Model. Softw..

[23]  Kozo H. Yoshida,et al.  A Subtropical Counter-Curreut in the North Pacific:An Eastward Flow Near the Subtropical Convergence , 1967 .

[24]  B. Qiu Seasonal Eddy Field Modulation of the North Pacific Subtropical Countercurrent: TOPEX/Poseidon Observations and Theory , 1999 .

[25]  Kerry A. Emanuel,et al.  The Interaction of Supertyphoon Maemi (2003) with a Warm Ocean Eddy , 2005 .

[26]  L. Oey Loop Current and Deep Eddies , 2008 .

[27]  L. Oey,et al.  Stalling of near‐inertial waves in a cyclone , 2008 .

[28]  Cheinway Hwang,et al.  TOPEX//Poseidon observations of mesoscale eddies over the Subtropical Countercurrent: Kinematic characteristics of an anticyclonic eddy and a cyclonic eddy , 2004 .

[29]  Jordi Font,et al.  Vortices of the Mediterranean Sea: An Altimetric Perspective , 2006 .

[30]  L. Oey Loop Current and Deep Eddies , 2008 .

[31]  H. Kawamura,et al.  Seasonal variation and instability nature of the North Pacific Subtropical Countercurrent and the Hawaiian Lee Countercurrent , 2002 .

[32]  W. White,et al.  Large-scale seasonal and secular variability of the subtropical front in the western North Pacific from 1954 to 1974 , 1978 .

[33]  H. Sakuma,et al.  The Kuroshio large meander formation in 2004 analyzed by an eddy‐resolving ocean forecast system , 2008 .

[34]  William E. Johns,et al.  The Kuroshio East of Taiwan: Modes of Variability and Relationship to Interior Ocean Mesoscale Eddies , 2001 .