Dynamics of the Antarctic circumpolar current : evidence for topographic effects from altimeter data and numerical model output
Dynamics of the Antarctic circumpolar current : evidence for topographic effects from altimeter data and numerical model output
Date
1995-02
Authors
Gille, Sarah T.
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publication.page.title.alternative
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Date Created
Location
Antarctic Circumpolar Current
Kerguelen Island
Campbell Plateau
Drake Passage
Kerguelen Island
Campbell Plateau
Drake Passage
DOI
10.1575/1912/5628
Replaced By
Keywords
Ocean currents
Eddy flux
Eddy flux
Abstract
Geosat altimeter data and numerical model output are used to examine the
circulation and dynamics of the Antarctic Circumpolar Current (ACC).
The mean sea surface height across the ACC has been reconstructed from
height variability measured by the Geosat altimeter, without assuming prior knowledge
of the geoid. For this study, an automated technique has been developed to
estimate mean sea surface height for each satellite ground track using a meandering
Gaussian jet model, and errors have been estimated using Monte Carlo simulation.
The results are objectively mapped to produce a picture of the mean Subantarctic
and Polar Fronts, which together comprise the major components of the ACC. The
locations of the fronts are consistent with in situ observations and indicate that the
fronts are substantially steered by bathymetry. The jets have an average Gaussian
width of about 44 km in the meridional direction and meander about 75 km to either
side of their mean locations. The width of the fronts is proportional to 1/f, indicating
that with constant stratification, the width is proportional to the baroclinic. Rossby
radius. The average height difference across the Subantarctic Front (SAF) is 0.7 m
and across the Polar Front (PF) 0.6 m. The mean widths of the fronts are correlated
with the size of the baroclinic Rossby radius. The meandering jet model explains
between 40% and 70% of the height variance along the jet axes. Bathymetric constrictions
are associated with increased eddy variability, a smaller percentage of which
may be explained by the meandering of the ACC fronts, indicating that propagating
eddies and rings may be spawned at topographic features.
Detailed examination of spatial and temporal variability in the altimeter data
indicates a spatial decorrelation scale of 85 km and a temporal e-folding scale of 34
days. The sea surface height variability is objectively mapped using these scales to
define autocovariance functions. The resulting maps indicate substantial evidence
of mesoscale eddy activity. Over 17-day time intervals, meanders of the PF and
SAF appear to elongate, break off as rings, and propagate. Statistical analysis of
ACC variability from altimeter data is conducted using empirical orthogonal functions
(EOFs ). The first mode EOF describes 16% of the variance in total sea surface
height across the ACC; reducing the domain into basin scales does not significantly
increase the variance represented by the first EOF, suggesting that the scales of motion are relatively short, and may be determined by local instability mechanisms
rather than larger basin scale processes. Likewise, frequency domain EOFs indicate
no statistically significant traveling wave modes.
The momentum balance of the ACC has been investigated using both output
from a high resolution primitive equation model and sea surface height measurements
from the Geosat altimeter. In the Semtner-Chervin general circulation model, run
with approximately quarter-degree resolution and time varying ECMWF winds, topographic
form stress is the dominant process balancing the surface wind forcing.
Detailed examination of form stress in the model indicates that it is due to three
large topographic obstructions located at Kerguelen Island, Campbell Plateau, and
Drake Passage. In order to reduce the effects of standing eddies, the model momentum
balance is considered in stream coordinates; vertically integrated through the
entire water column, topographic form drag is the dominant balance for wind stress.
However, at mid-depth the cross-stream momentum transfer is dominated by horizontal
biharmonic friction. In the upper ocean, horizontal friction, mean momentum
flux divergence, transient momentum flux divergence, and mean vertical flux divergence
all contribute significantly to the momentum balance. Although the relative
importance of individual terms in the momentum balance does not vary substantially
along streamlines, elevated levels of eddy kinetic energy are associated with the three
major topographic features. In contrast, altimeter data show elevated energy levels
at many more topographic features of intermediate scales, suggesting that smaller
topographic effects are better able to communicate with the surface in the real ocean
than in the model. Transient Reynolds stress terms play a small role in the the
overall momentum balance; nonetheless, altimeter and model measurements closely
agree, and suggest that transient eddies tend to accelerate the mean flow, except in
the region between the major fronts which comprise the ACC.
Potential vorticity is considered in the model output along Montgomery streamfunction.
Even at about 1000 m depth, it varies in response to wind forcing, largely as
a result of changes in vertical stratification, indicating that forcing and dissipation do
not locally balance in the Southern Ocean. In order to compare model and altimeter
potential vorticity estimates, two different proxies for potential vorticity on surface
streamlines are considered. Both proxies show very similar results for model and altimeter,
suggesting that differences in surface streamlines estimated by the altimeter
and the model are not significant in explaining the Southern Ocean flow. The proxies
are both roughly conserved along surface height contours but undergo substantial
jumps near topographic features. However, they cannot capture stratification changes
which may be critically important to the overall potential vorticity balance.
Description
Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy at the Massachusetts Institute of Technology and the Woods Hole Oceanographic Institution February 1995