WIND-DRIVEN COASTAL GENERATION OF ANNUAL MESOSCALE EDDY ACTIVITY IN THE CALIFORNIA CURRENT

Citation
A. Paressierra et al., WIND-DRIVEN COASTAL GENERATION OF ANNUAL MESOSCALE EDDY ACTIVITY IN THE CALIFORNIA CURRENT, Journal of physical oceanography, 23(6), 1993, pp. 1110-1121
Citations number
27
Categorie Soggetti
Oceanografhy
ISSN journal
00223670
Volume
23
Issue
6
Year of publication
1993
Pages
1110 - 1121
Database
ISI
SICI code
0022-3670(1993)23:6<1110:WCGOAM>2.0.ZU;2-D
Abstract
Two candidate sources for the generation of mesoscale eddy activity in the California Current are local baroclinic instability and/or the wi nd stress adjacent to the coast. The latter constitutes remote forcing , with eddy activity propagating westward from the coast into the Cali fornia Current via Rossby wave dynamics. In this study, two wind-drive n models are utilized to test the relative significance of these two s ources. One is an eddy resolving quasigeostrophic (QG) model, with the ability to represent baroclinic instability but not the coastal respo nse to winds. The other is a 1 1/2-layer primitive equation (PE) model with the ability to represent the coastal response to winds but not b aroclinic instability. Both models have the same spatial grid (i.e., a pproximately 20 km) and are driven by the same coarse-grid wind-stress forcing fields over the same one-year time period (i.e., January 1987 to December 1987). This period is chosen because of the availability of Geosat altimetric sea-level observations with which to verify these models. Earlier, White and colleagues analyzed these same altimetric sea-level observations, finding dominant mesoscale eddy activity occur ring on wavelength scales of 400-800 km and period scales of 6-12 mont hs. This mesoscale variability propagates to the west at 2-5 cm s-1, f aster at lower latitude, consistent with Rossby wave dynamics. Moreove r, the eddy variance is largest next to the coast, maximum between Mon terey and Cape Mendocino, and southwest of Point Conception. The PE mo del is able to simulate qualitatively this distribution of the eddy va riance as it appears in altimetric sea level, yielding significant coh erence and phase between model and observed sea-level residuals along longitude/time matrices at 30-degrees-N and 40-degrees-N. The QG model , on the other hand, is found incapable of simulating the main feature s of this distribution of eddy variance. The reason for the agreement between the PE model and the satellite altimetric sea-level observatio ns is that the dominant source of mesoscale eddy activity on these tim e and space scales is the wind forcing adjacent to the coast, modified by both Rossby and Kelvin wave dynamics.