Large-scale propagating disturbances: Approximation by vertical normal modes

Citation
Pd. Killworth et Jr. Blundell, Large-scale propagating disturbances: Approximation by vertical normal modes, J PHYS OCEA, 31(10), 2001, pp. 2852-2870
Citations number
40
Categorie Soggetti
Aquatic Sciences","Earth Sciences
Journal title
JOURNAL OF PHYSICAL OCEANOGRAPHY
ISSN journal
00223670 → ACNP
Volume
31
Issue
10
Year of publication
2001
Pages
2852 - 2870
Database
ISI
SICI code
0022-3670(2001)31:10<2852:LPDABV>2.0.ZU;2-P
Abstract
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.