The energetics and tidally induced reverse renewal in a two-silled fjord

Citation
Mw. Stacey et Y. Gratton, The energetics and tidally induced reverse renewal in a two-silled fjord, J PHYS OCEA, 31(6), 2001, pp. 1599-1615
Citations number
27
Categorie Soggetti
Aquatic Sciences","Earth Sciences
Journal title
JOURNAL OF PHYSICAL OCEANOGRAPHY
ISSN journal
00223670 → ACNP
Volume
31
Issue
6
Year of publication
2001
Pages
1599 - 1615
Database
ISI
SICI code
0022-3670(2001)31:6<1599:TEATIR>2.0.ZU;2-I
Abstract
A laterally integrated, two-dimensional numerical model is used to examine the influence of the M-2 tide on the circulation in the Saguenay Fjord, a t wo-silled fjord (with a "large'' inner and a "small'' outer basin) located on the north shore of the St. Lawrence Estuary. It is found that the M-2 ti de is more vigorous in the outer than in the inner basin and that more vert ical mixing occurs in the outer basin. Therefore, the density at depth in t he outer basin decreases faster than it does in the inner basin, and the re sulting horizontal pressure gradient causes a bottom flow of water from the inner to the outer basin across the inner sill. This "reverse renewal'' is evident in both the available observations and the simulation. According to the model, much of the M-2 energy withdrawn from the surface t ide is fed into the internal tide. Significant tidal energy is also advecte d by the mean flow velocity. Approximately 25% of the net energy flux into the fjord is dissipated within 2 km of the outer sill. Because of the baroclinic pressure (i.e., the total pressure but with the i nfluence of the surface displacement removed) the subtidal circulation is a ssociated with very large energy fluxes within the fjord. These fluxes are much larger than the net rate at which tidal energy enters the fjord and th ey are greater than the subtidal, advective energy flux. They represent a l arge redistribution of energy within the fjord and their horizontal diverge nce along the fjord is almost in balance with the time rate of change of po tential energy. When a flux Richardson number is calculated for the inner basin below sill depth, a value of 0.075 is obtained, which is close to values found for oth er fjords.