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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(1) The upwelled horizontal pr<strong>of</strong>iles <strong>of</strong> surface layer<br />
density scale with the initial internal deformation radii.<br />
The upwelling process (in this simple model) rotates the<br />
vertical density pr<strong>of</strong>ile to the horizontal <strong>and</strong> stretches it<br />
by a factor <strong>of</strong> the order <strong>of</strong> an initial deformation radius.<br />
(2) There is surface transport divergence around the<br />
upwelling fronts <strong>of</strong> the same magnitude as the divergence in<br />
the upwelling zone adjacent to the coastal boundary. (The<br />
magnitude is roughly the <strong>of</strong>fshore Ekman transport divided by<br />
the local internal deformation radius associated with the<br />
mixed layer base.) However, this divergence is associated<br />
only with the deformation <strong>of</strong> the mixed layer base near the<br />
moving fronts. Interior stratification inhibits the depth<br />
penetration <strong>of</strong> the local divergence around the <strong>of</strong>fshore<br />
front, <strong>and</strong> upwelling <strong>of</strong> the deep interior occurs only at the<br />
coastal boundary.<br />
The model retains the essential physics <strong>of</strong> wind-driven<br />
thermocline upwelling. However, it has limitations. Any<br />
attempt to directly model specific oceanic conditions must<br />
take alongshore variability into account. The neglect <strong>of</strong><br />
inertio-gravity waves forces the instantaneous establishment<br />
<strong>of</strong> the modified Ekman balance far <strong>of</strong>fshore <strong>and</strong> shortens the<br />
upwelling time scales. The inclusion <strong>of</strong> shear mixing in the<br />
entrainment parameterization would lead to reduced velocities<br />
in the geostrophic jets.<br />
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