Observations and Modelling of Fronts and Frontogenesis
Observations and Modelling of Fronts and Frontogenesis
Observations and Modelling of Fronts and Frontogenesis
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interior layers, on the horizontal scale <strong>of</strong> the local<br />
internal deformation radius.<br />
The uppermost interior layer eventually becomes<br />
entrained completely into the surface layer in the upwelling<br />
region, leaving only two layers there. We derive matching<br />
conditions to join the two-layer region with the three-layer<br />
region. Sustained upwelling results in a step-like<br />
horizontal pr<strong>of</strong>ile <strong>of</strong> surface layer density, as the interior<br />
layer interface "surfaces" <strong>and</strong> is advected <strong>of</strong>fshore as a<br />
front in the surface layer. The upwelled horizontal density<br />
pr<strong>of</strong>ile scales with an internal deformation radius calculated<br />
from the initial fields.<br />
III.2.a Equations<br />
111.2 Model formulation<br />
Figure 111.1 displays the model geometry. We use a<br />
right-h<strong>and</strong>ed Cartesian coordinate system with origin at the<br />
surface on the coastal boundary, x alongshore, y positive<br />
<strong>of</strong>fshore, <strong>and</strong> z vertical. We specify that all flow variables<br />
be uniform in the alongshore direction <strong>and</strong> take the flow to<br />
be governed by the semigeostrophic equations (e.g. , Pedlosky,<br />
1979, Sec. 8.4): the geostrophic balance holds normal to<br />
shore, while the alongshore acceleration is retained at<br />
lowest order. The main effect <strong>of</strong> imposing semigeostrophy is<br />
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