2018
DOI: 10.1088/1361-6544/aaaf2d
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Periodic solutions with prescribed minimal period of vortex type problems in domains

Abstract: We consider Hamiltonian systems with two degrees of freedom of point vortex typefor z 1 , z 2 in a domain Ω ⊂ R 2 . In the classical point vortex context the Hamiltonian H Ω is of the formwhere g : Ω × Ω → R is the regular part of a hydrodynamic Green's function in Ω, h : Ω → R is the Robin function: h(z) = g(z, z), and κ 1 , κ 2 are the vortex strengths. We prove the existence of infinitely many periodic solutions with prescribed minimal period that are superpositions of a slow motion of the center of vortici… Show more

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Cited by 4 publications
(4 citation statements)
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“…A generalized analysis of Leapfrogging vortex rings have been also discussed in [15,22,23,43,52] and the references therein. In addition to the leapfrogging motion, many periodic non-rigid configuration of vortex point system set in a general domain were also discussed in [4,5,36,55]. Very recently, time quasi-periodic solutions have been explored for Euler equations around the ellipses [12] or around the Rankine vortices in the disc [40].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…A generalized analysis of Leapfrogging vortex rings have been also discussed in [15,22,23,43,52] and the references therein. In addition to the leapfrogging motion, many periodic non-rigid configuration of vortex point system set in a general domain were also discussed in [4,5,36,55]. Very recently, time quasi-periodic solutions have been explored for Euler equations around the ellipses [12] or around the Rankine vortices in the disc [40].…”
Section: Introductionmentioning
confidence: 99%
“…The second equation in (1) is nothing but the Biot-Savart law which can be written in the complex form:…”
mentioning
confidence: 99%
“…In the first one vortices with possibly different strengths and of arbitrary number are close to a critical point of the so called Robin function h Ω (z) = g Ω (z, z) and the configuration of vortices looks after rescaling like a rigidly rotating solution of the N -vortex system on R 2 , see [4,6]. In the second type of solutions, shown in [10], two identical vortices rotate around their center of vorticity while the center itself follows a level line of h Ω . The third result holds for an arbitrary number of identical vortices, which separated by time shifts follow the same curve close to the boundary of a simply connected bounded domain, [5].…”
Section: Introduction and Statement Of Resultsmentioning
confidence: 99%
“…In general domains Ω ⊂ R 2 , the Hamiltonian H Ω does not share the advantages of the cases stated above. Still, using perturbative approaches the existence of some types of periodic solutions could also be established in general domains [3,4,5,8,15]. In recent years, also different kinds of stationary solutions, i.e.…”
Section: Introductionmentioning
confidence: 99%