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The large-scale spatial pattern of sea surface height variability is captured
by the model (see Fig. 15-17). The North Atlantic Current extends through the
southeast corner of the model domain and is associated with very large
variability in sea surface height. The model captures roughly 75 percent of the
energy in this region despite the proximity to the model boundary. In fact, the
boundary conditions only give abnormally low variability within the sponge
layer (nearest 5 grid points to the the boundary) without a noticeable effect
to the interior. For the year of Oct. 1996-1997, the Topex/Poseidon altimeter
observes a maximum SSH variance of nearly
in the western boundary
current extension, while the model predicts maximum values of
. The
model also correctly gives lower variability in the center of the Labrador Sea.
The point-by-point correlation coefficient between model and altimetry SSH
variance in the entire model domain is .75, primarily due to the model's
ability to distinguish between high variability in the North Atlantic Current
and lower variability in the Labrador Sea proper. However, a closer look at
the center of the Labrador Sea reveals slightly more ambiguous results. In this
area, the model only captures 40-50 percent the total SSH variance. The spatial
mean SSH variance is
in the model,
in the altimetry
data. Next, the model predicts a local maximum variance in the rim current of
, but much smaller variability in the center of the Labrador Sea's
convecting area. The altimeter also sees a slight maximum in the rim current,
but there is almost the same amount of variability in the center of the
Labrador Sea. The model's spatial pattern is not quite as good in this smaller
region, despite its successes on the large scale. The signal in the data is
much larger than the noise , which is estimated to be on the order of
(Fu et al, 1994) and can not possibly explain the discrepancy in the
center of the Labrador Sea. It has been speculated that lack of model
resolution is responsible for the low background variability away from frontal
structures (Stammer and Boning, 1996). This seems to be a logical explanation
in regions of convection since such small spatial scales can not be explicitly
seen even by this relatively high resolution model. However , this model is
eddy-resolving and we should see more variability than lower resolution models
if this hypothesis is correct. Indeed, previous studies with 2 degree
resolution global GCM's only capture 25-50 percent of the sea surface height
variance (Stammer et al, 1996). In energetic regions such as the West Greenland
rim current and the North Atlantic Current, this model consistently captures at
least 75 percent of the variability. Although sea surface height variability in
the convective region is not captured to the same degree, perhaps this should
be expected by a model which does not explicitly resolve such small
features. The degree of resolution needed can be more adequately discussed
after a study of the frequency spectra.
Next: SSH Frequency Spectra
Up: Sea Surface Height
Previous: Sea Surface Height
Jake Gebbie
2003-04-10