Abstract

Abstract The equatorial deep jets are often modeled as equatorially trapped long waves, either Kelvin or Rossby. Rossby waves perturb potential vorticity but Kelvin waves do not; therefore the potential vorticity structure of a 16-month mean velocity section from 3°N to 3°S on 159°W is examined. To distinguish the equatorial deep jets from flow components with larger vertical scales, the mean profiles were decomposed into a low-vertical-mode component and a residual, dominated by the deep jets. The deep jets resemble a first-meridional-mode Rossby wave; their velocity at 2°N and 2°S is opposite in direction to their velocity on the equator, and consequently they show a potential vorticity perturbation. The zero crossings of the jets zonal velocity are at 1°30′N and S, farther from the equator than the 1°N and S predicted by linear wave theory. One possible explanation for this broadening is meridional advection of the jets by higher-frequency motions such as Rossby–gravity waves.

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