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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 />

L9

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