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Next: 4.2.3.2 Horizontal pressure gradient Up: 4.2.3 Horizontal momentum equations Previous: 4.2.3 Horizontal momentum equations

4.2.3.1 Coriolis force

The Coriolis force

$\displaystyle {\bf F}_{C} = {\bf u} \wedge f \, \hat{z} = f(v,-u,0)$     (4.14)

arises from writing the equations in the rotating reference frame of the earth. This force does zero work on the fluid, since ${\bf u}
\cdot {\bf F}_{C} = 0$. In the northern hemisphere, this force acts to the right of the fluid velocity vector, and in the south, it acts to the left.



RC Pacanowski and SM Griffies, GFDL, Jan 2000