Summary
The planar motion ofN inviscid point vortices in the presence of a fixed rigid obstacle is described by an autonomous Hamiltonian set of differential equations. For circular and rectilinear boundary of the obstacle the two-vortex system is integrable. Numerical simulations suggest that the perturbation of the circular boundary into an ellypse causes homoclinic bifurcation in the restricted two-vortex system and transition to chaotic motion. This may be compared with the case of systems of free vortices (no obstacle) where chaotic motion first appears atN=4.
Similar content being viewed by others
References
L. M. Milne-Thomson:Theoretical Hydrodynamics (McMillan, 1967).
A. I. Markusevich:Theory of Functions of a Complex Variable (Prentice Hall, 1981).
V. I. Arnold:Mathematical Methods of Classical Mechanics (Springer-Verlag, 1983).
H. Aref:Phys. Fluids,22, 393 (1979).
H. Aref andN. Pomphrey:Proc. R. Soc. London,380, 359 (1982).
E. A. Novikov:Sov. Phys. JETP (Engl. Transl.),41, 937 (1975).
E. A. Novikov andY. B. Sedow:JETP Lett.,29, 677 (1979).
J. Guckenheimer andP. Holmes:Nonlinear Oscillations, Dynamical Systems and Bifurcations of Vector Fields (Springer-Verlag, 1986).
Author information
Authors and Affiliations
Additional information
The authors of this paper have agreed to not receive the proofs for correction.
Rights and permissions
About this article
Cite this article
Lupini, R., Siboni, S. Chaotic motions of inviscid point vortices around rigid obstacles. Nuov Cim B 106, 957–962 (1991). https://doi.org/10.1007/BF02728339
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02728339