Meridional transport of salt in the global ocean from an eddy-resolving model

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Abstract

The meridional transport of salt is computed in a global eddy-resolving numerical model (1/12° resolution) in order to improve our understanding of the ocean salinity budget. A methodology is proposed that allows a global analysis of the salinity balance in relation to surface water fluxes, without defining a "freshwater anomaly" based on an arbitrary reference salinity. The method consists of a decomposition of the meridional transport into (i) the transport by the time-longitude-depth mean velocity, (ii) time-mean velocity recirculations and (iii) transient eddy perturbations. Water is added (rainfall and rivers) or removed (evaporation) at the ocean surface at different latitudes, which creates convergences and divergences of mass transport with maximum and minimum values close to ±1 Sv. The resulting meridional velocity effects a net transport of salt at each latitude (±30 Sv PSU), which is balanced by the time-mean recirculations and by the net effect of eddy salinity-velocity correlations. This balance ensures that the total meridional transport of salt is close to zero, a necessary condition for maintaining a quasi-stationary salinity distribution. Our model confirms that the eddy salt transport cannot be neglected: it is comparable to the transport by the time-mean recirculation (up to 15 Sv PSU) at the poleward and equatorial boundaries of the subtropical gyres. Two different mechanisms are found: eddy contributions are localized in intense currents such as the Kuroshio at the poleward boundary of the subtropical gyres, while they are distributed across the basins at the equatorward boundaries. Closer to the Equator, salinity-velocity correlations are mainly due to the seasonal cycle and large-scale perturbations such as tropical instability waves.

Figures

  • Fig. 1. Top panel: evaporation–precipitation–runoff flux for the global ORCA12 model (kgm−2 s−1). Positive values correspond to regions where evaporation is dominant. Bottom panel: salinity (PSU) averaged over the top 200 m in the ORCA12 model. It is a time–mean over the last 10 years of an 85 year-long experiment.
  • Fig. 2. Box model used to introduce the salt transport decomposition. (a) schematic of the exchanges between the two boxes a short time into the spin-up (typically days or weeks). A barotropic flux F0 is set up to carry the excess mass input into the subpolar box by precipitations, in order to avoid indefinite growth of the difference in sea level between the two boxes. It induces a barotropic transport of salt (noted as v0S0, green arrow); (b) schematic of the exchanges between the boxes at equilibrium. Salinity anomalies S∗ develop as a consequence of the barotropic salt flux. Three-dimensional recirculations are established over long timescales (years, decades) which carry salinity anomalies (the transport is noted v∗S∗, red arrow). At equilibrium the salt content of each box is constant and the salt flux v∗S∗ due to the recirculation cancels the salt flux v0S0 carried by the barotropic volume flux F0.
  • Fig. 4. Decomposition of the global meridional transport of salt in the ORCA12 simulation. See text (Eq. 8) for the explanation of the different terms. The grey shading is the observed salt flux carried by the net volume flux at each latitude: it is computed from the data of Large and Yeager (2009) (similar to Fig. 3) combined with the Levitus depth-averaged salinity field.
  • Fig. 3. Meridional transport resulting from the surface water flux in the ORCA12 model (Sv, thick black line), and comparison with Large and Yeager (2009). The grey shading is the envelope of all annual transports resulting from the air–sea fluxes of Large and Yeager (2009) for years 1984 to 2006 (these fluxes are a combination of observations and the NCEP reanalysis). The thin black line is the meridional transport computed directly from the model meridional velocities.
  • Fig. 5. Further analysis of the meridional transport of salt in the ORCA12 simulation. Top panel: transport by the time–mean recirculation velocity (thin black curve, same as Fig. 4), and its two components: the “overturning” (transport by the zonally averaged, depth-dependent velocity) and the “gyre” component. Bottom panel: contributions from the model drift and the ice–ocean flux which could explain the non-zero total salt transport (the red curve, same as in Fig. 4).
  • Fig. 6. Eddy and seasonal contributions to the meridional transport of salt in the ORCA12 simulation.
  • Fig. 7. Divergence of the eddy salt transport in the ORCA12 simulation, computed for 12× 12 grid point boxes to enhance readability. It is integrated vertically and thus expressed in units of PSUms−1. The colour scale is saturated in the red and blue at 5×10−6 PSUms−1 (the maxima and minima of the field are about 40 times larger). Top panel: total eddy component; bottom panel: seasonal contribution only.

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CITATION STYLE

APA

Treguier, A. M., Deshayes, J., Le Sommer, J., Lique, C., Madec, G., Penduff, T., … Talandier, C. (2014). Meridional transport of salt in the global ocean from an eddy-resolving model. Ocean Science, 10(2), 243–255. https://doi.org/10.5194/os-10-243-2014

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