Interaction of a monopolar vortex with a topographic ridge
J.H.G.M. van Geffen and P.A. Davies
Geophys. & Astrophys. Fluid Dynam. 90, 1--41 (1999)
abstract
The interaction of a monopolar vortex with a cosine-shaped topographic ridge
at the equator is investigated with a two-dimensional numerical model, where
the (cyclonic) monopole has a self-induced northwest-ward motion due to the
beta-effect.
The fate of the monopole depends on the width and height of the ridge, but,
more importantly, on the orientation of the ridge.
Whereas monopoles are always seen to cross an east-west or
northeast-southwest ridge, a north-south ridge can cause such deformations
in the monopole's shape that it either splits into two parts (where the
associated secondary vortex may or may not also cross the ridge) or it is
destroyed.
The computations show that the monopole can only cross the top of the ridge
once it has gathered sufficient positive potential vorticity at its
(north)west side. The vortex achieves this by moving along the ascending
side of the ridge, westward for the east-west ridge and northward for the
north-south ridge, before crossing the summit.
1. Introduction
2. The numerical model
2.1 Governing equations
2.2 Numerical method
3. Basic effects of a bottom topography
3.1 A Lamb dipole crossing a ridge
===> Web page
4. The monopole used for the interaction-study
4.1 A Bessel monopole on a pure beta-plane
===> Web page
5. A ridge along the x-axis
6. A ridge along the line y=x
7. A ridge along the y-axis
7.1 A ridge with A=0.20 and w=1.0
===> Web page
7.2 Ridges of different widths
7.3 Effect of a lower viscosity
7.4 Ridges with different heights
8. Concluding remarks
Acknowledgments
References
Full paper (2.2B)
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