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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divergence in the mixed layer <strong>and</strong> convergence in the<br />
interior, resulting in upwelling <strong>of</strong> isopycnals near the<br />
coast. The horizontal scale over which this upwelling occurs<br />
adjusts dynamically according to (28).<br />
were,<br />
The initial conditions for the cases reported on here<br />
h10 - 0.5 [17m] , h20 = 1.0 [33 ml,<br />
ulO=u20=u30=O,<br />
with total depth H = 10 [330 m] <strong>and</strong> density differences,<br />
Case 1: 2l - 1000 [0.3 kg m3],<br />
(38)<br />
32 - 100 [0.03 kg m3] , (39a)<br />
Case 2: 2l = 5000 [1.5 kg m3],<br />
'32 = 500 [0.15 kg m3] , (39b)<br />
Case 3: 2l 10000 [3 kg m3],<br />
32 = 1000 [0.3 kg m3]. (39c)<br />
In all cases, the forcing was constant,<br />
r = - 1 [0.1 N m2], Q 1 [75 W m2], (40)<br />
<strong>and</strong> the total depth H 10 [330 ml. In the following<br />
discussion, we focus on Case 1. When dimensional values<br />
depend on the density differences, we give only the<br />
dimensional values corresponding to Case 1.<br />
Initially, when the layer depths <strong>and</strong> density differences<br />
are independent <strong>of</strong> y <strong>and</strong> the geostrophic velocities vanish<br />
identically, the system (28) with (17) may be solved