The dynamics of Lagrangian particles and tracers, in the vicinity of a baro
clinically unstable zonal jet are investigated in a simple two-layer model
with an initially quiescent lower layer. The presence of a growing wave ind
uces a particle drift dominated by Stokes drift rather then the contributio
n of the wave to the mean Eulerian velocity. Stable and unstable waves have
zonal Stokes drift with similar meridional structure while only unstable w
aves possess meridional drift, which is in the direction of increasing meri
dional wave displacement. Particle dispersion in the upper layer is maximum
at critical lines, where the jet and phase speeds are equal. in the lower
layer, dispersion is maximum where the wave amplitude is maximum. Zonal mea
n tracer evolution is formulated as an advection-diffusion equation with an
order Rossby number advection and an order-one eddy diffusion. The latter
is proportional to two-particle dispersion.
Finite amplitude simulations of the flaw reveal that small amplitude theory
has predictive value beyond the range for which it is strictly valid. Mixi
ng (as opposed to stirring) is maximum near cat's-eye-like recirculation re
gions at the critical line's. In the lower layer the pattern of convergence
and divergence of the flow locally increases tracer gradients, resulting i
n stirring yet with a much slower mixing rate than in the upper layer. Meri
dional eddy diffusion (or particle dispersion) alone is not sufficient for
prediction of mixing intensity. Rotation, which is quantified by the cross-
correlation of meridional and zonal displacements, must also be present for
mixing.
These results are consistent with observations of tracer and floats in the
vicinity of the Gulf Stream.