| The following results are taken from Padman et al. (2005).
So far, we have assumed that tidal currents are constant with depth. This
is often a fairly good approximation in Antarctic seas. However, sometimes
we need to worry about “baroclinic” tides. These are tidal
currents that exists because of stratification in the ocean. Here is an
example of what baroclinicity does to the tidal currents. |
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The left hand plot shows how ocean density changes with
depth. Here, we basically have a 2-layer ocean, with a density gradient
(or “pycnocline”) between 200 and 400 m depth. The effect
is, when tides flow across steep topography like the South Scotia Ridge,
the interface acts a bit like the ocean surface, and a wave is generated
that travels along the pycnocline. The result is much greater variability
of surface currents and divergence than you get in a depth-averaged
model. |
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Below, we look at the map of divergence
for the northern Weddell Sea, comparing a depth-averaged model with
a 3-D model based on much more complicated equations of fluid motion.
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We find that the generation of internal
tides along the South Scotia Ridge in a 3-D ocean tidal model leads
to much higher ice divergence than for the case of depth-averaged currents.
Instead of the rms divergence being about 2% along the ridges, we get
values that frequently exceed 10%. |
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Using 3-D rather than depth-averaged models slows down
the modeling effort by a couple of orders of magnitude. However, as
this example shows, it will be necessary to do this in order to get
the effect of ocean tides on sea ice right. |