On wind-driven energetics of subtropical gyres
<p>The flow of energy in the wind-driven circulation is examined in a&#160;<br>combined theoretical and numerical study. Based on a multiple scales&#160;<br>analysis of the ocean interior, we find the mesoscale field is strongly&#160;<br>affected by the ventilated thermocline, but no feed back from the eddies&#160;<br>to the large scale is found. &#160;We then analyze the western boundary&#160;<br>region arguing that the associated currents divide between coastal jets,&#160;<br>which conserve mean energy, and open ocean, separated jet extensions<br>where the mesoscale is energized by the mean field. &#160; It is the&#160;<br>separated jet zone where the primary loss of general circulation energy&#160;<br>to the mesoscale occurs. &#160;Connections to the `Thickness Weighted&#160;<br>Average' form of the primitive equations are made which support the&#160;<br>differing roles of the eddies in these regions. &#160;These ideas are then&#160;<br>tested by an analysis of a regional primitive equation 1/12-degree&#160;<br>numerical model of the North Atlantic. The predictions of the theory are&#160;<br>generally supported by the numerical results. &#160;The one exception is that&#160;<br>topographic irregularities in the coastal jet spawn eddies, although&#160;<br>they contribute modestly to the energy budget. &#160;We therefore conclude&#160;<br>the primary sink of wind input into the mean circulation is in the&#160;<br>separated jet, and not the interior. &#160;The analysis also shows<br>wind forcing is much smaller than the interior energy fluxes. Thus, the&#160;<br>general circulation is characterized as recirculating energy in the&#160;<br>manner of a Fofonoff gyre.</p>