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Observations and Modelling of Fronts and Frontogenesis

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111.1 Introduction<br />

In this chapter we combine a simple representation <strong>of</strong> a<br />

stratified interior with a previously-developed theory for<br />

strong horizontal gradients in a surface mixed layer (de<br />

Szoeke <strong>and</strong> Richman, 1984) to develop a model for the wind-<br />

driven upwelling <strong>of</strong> a stratified fluid. We apply the model<br />

to the case <strong>of</strong> coastal upwelling. The interior consists <strong>of</strong><br />

two homogeneous layers <strong>of</strong> differing density. The mixed layer<br />

resolves the fronts that form as layer interfaces "surface"<br />

at the coast <strong>and</strong> are advected <strong>of</strong>fshore. Combining these<br />

elements allows the modelling <strong>of</strong> the upwelling <strong>and</strong><br />

entrainment into the surface layer <strong>of</strong> deep, dense interior<br />

fluid that is initially separated from the surface layer by<br />

an intermediate layer <strong>of</strong> less-dense fluid.<br />

We employ two principal analytical simplifications: we<br />

specify that all flow variables be uniform in the alongshore<br />

direction, <strong>and</strong> that semigeostrophic dynamics apply.<br />

These semigeostrophic equations are similar to those<br />

developed by Hoskins <strong>and</strong> Bretherton (1972) for the study <strong>of</strong><br />

atmospheric frontogenesis (subsequently generalized to three<br />

dimensions by Hoskins (1975)). They were used by Pedlosky<br />

(1978) in an adiabatic model <strong>of</strong> the onset <strong>of</strong> upwelling driven<br />

by a mass sink at the coast <strong>and</strong> an alongshore pressure<br />

gradient.<br />

47

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