Propagating features and waves occur everywhere in the ocean. This paper de
rives a concise description of how such small-amplitude, large-scale oceani
c internal disturbances propagate dynamically against a slowly varying back
ground mean flow and stratification, computed using oceanic data. For a fla
t-bottomed ocean, assumed here, the linear internal modes, computed using t
he local stratification, form a useful basis for expanding the oceanic shea
r modes of propagation. Remarkably, the shear modal structure is largely in
dependent of orientation of the flow. The resulting advective velocities, w
hich are termed pseudovelocities, comprise background flow decomposed onto
normal modes, and westward planetary wave propagation velocities. The diago
nal entries of the matrix of pseudovelocities prove to be reasonably accura
te descriptors of the speed and direction of propagation of the shear modes
, which thus respond as if simply advected by this diagonal-entry velocity
field. The complicated three-dimensional propagation problem has thus been
systematically reduced to this simple rule.
The first shear mode is dominated by westward propagation, and possesses a
midlatitude speed-up over the undisturbed linear first-mode planetary wave.
The pseudovelocity for the second shear mode, in contrast, while still dom
inated by westward propagation at lower latitudes, shows a gyrelike structu
re at latitudes above 30 degrees. This resembles in both shape and directio
n the geostrophic baroclinic flow between about 500- and 1000-m depth, but
are much slower than the flow at these depths. Features may thus be able to
propagate some distance around a subtropical or subpolar gyre, but not, in
general, at the speed of the circulation.