Dynamics of the Pacific Subsurface Countercurrents*

Abstract

A hierarchy of models, varying from 2 -layer to 4 -layer systems, is used to explore the dynamics of the 11 22 Pacific Subsurface Countercurrents, commonly referred to as ‘‘Tsuchiya Jets’’ (TJs). The TJs are eastward currents located on either side of the equator at depths from 200 to 500 m and at latitudes varying from about 28 to 78 north and south of the equator, and they carry about 14 Sv of lower-thermocline (upper-intermediate) water throughout the tropical Pacific. Solutions are found in idealized and realistic basins and are obtained both analytically and numerically. They are forced by winds and by a prescribed Pacific interocean circulation (IOC) with transport M (usually 10 Sv), representing the outflow of water in the Indonesian passages and a compensating inflow from the Antarctic Circumpolar Current. Analytic solutions to the 2 -layer model suggest that the TJs are geostrophic currents along arrested fronts. 1 2 Such fronts are generated when Rossby wave characteristics, carrying information about oceanic density structure away from boundaries, converge or intersect in the interior ocean. They indicate that the southern and northern TJs are driven by upwelling along the South American coast and in the ITCZ band, respectively, that the northern TJ is strengthened by a recirculation gyre that extends across the basin, and that TJ pathways are sensitive to stratification parameters. Numerical solutions to the 2 -layer and 4 -layer models confirm the analytic results, 11 22 demonstrate that the northern TJ is strengthened considerably by unstable waves along the eastward branch of the recirculation gyre, show that the TJs are an important branch of the Pacific IOC, and illustrate the sensitivity of TJ pathways to vertical-mixing parameterizations and the structure of the driving wind. In a solution to the 2 -layer model with M 5 0, the southern TJ vanishes but the northern one remains, being 1 2 maintained by the unstable waves. In contrast, both TJs vanish in the M 5 0 solution to the 4 -layer model,