09.04.2013 Views

Observations and Modelling of Fronts and Frontogenesis

Observations and Modelling of Fronts and Frontogenesis

Observations and Modelling of Fronts and Frontogenesis

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

to remove the inertio-gravity waves. The momentum <strong>and</strong><br />

continuity equations are, in the surface mixed layer (layer<br />

1),<br />

ult + Viuly - fv1 TZ/P0 = (TX re)/pOhl, (la)<br />

fu1 = /POi (lb)<br />

Plz = - gp(y,t),<br />

vly + wlz = 0,<br />

<strong>and</strong> in the interior layers (layers 2 <strong>and</strong> 3),<br />

(ic)<br />

(ld)<br />

uit + ViUiy fv 0, (2a)<br />

fui Piy/P0 (2b)<br />

Pjz = gpj. (2c)<br />

Viy + = 0, i=2,3. (2d)<br />

Here (ui,vi,wi) are the (x,y,z) components <strong>of</strong> velocity <strong>and</strong> Pj<br />

is density in layer i, i = 1,2,3, p is pressure, h1 is the<br />

depth <strong>of</strong> the mixed layer, P0 is a constant reference density,<br />

f is the Coriolis parameter, <strong>and</strong> g is the acceleration <strong>of</strong><br />

gravity. Subscripts x, y, <strong>and</strong> z denote partial<br />

differentiation. The upper layer density p is allowed to<br />

vary with y <strong>and</strong> t, while the interior layer densities are<br />

constant. The angle brackets around the upper layer pressure<br />

gradient denotes a vertical average through the mixed layer.<br />

This allows the neglect <strong>of</strong> the vertical shear that is<br />

associated with horizontal density gradients through the<br />

thermal wind relation. (This procedure can be justified as<br />

in de Szoeke <strong>and</strong> Richman (1984) by an expansion in orthogonal<br />

50

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!