| Situation | Coriolis force | The velocity | The vorticity |
| non-equational | consider | $ (0,0,0) $ | $ (0,0,0) $ |
| equational | don't consider | $ (u,v,w) $ | $ (0,\Omega_{2},0) $ |
We study the geophysical fluid dynamical problem of the wind in the steady atmospheric Ekman layer with constant eddy viscosity. Three dimensional Ekman flows with constant vorticity is considered in the $ f- $plane approximation. For non-equatorial $ f- $plane approximation, we show that any bounded solution of the Ekman flow with a flat surface and constant vorticity vector is the stationary flow with vanishing velocity field, while for the equatorial $ f- $plane approximation, we obtain that the pressure presents no variation in the northward direction and the meridional component is constant throughout the fluid domain.
| Citation: |
Table 1.
A comparison between the non-equatorial and the equatorial
| Situation | Coriolis force | The velocity | The vorticity |
| non-equational | consider | $ (0,0,0) $ | $ (0,0,0) $ |
| equational | don't consider | $ (u,v,w) $ | $ (0,\Omega_{2},0) $ |
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The flow domain