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The stability around Chariklo and the confinement of its rings

dc.contributor.authorGiuliatti Winter, S. M. [UNESP]
dc.contributor.authorMadeira, G. [UNESP]
dc.contributor.authorRibeiro, T. [UNESP]
dc.contributor.authorWinter, O. C. [UNESP]
dc.contributor.authorBarbosa, G. O. [UNESP]
dc.contributor.authorBorderes-Motta, G.
dc.contributor.institutionUniversidade Estadual Paulista (UNESP)
dc.contributor.institutionCNRS
dc.contributor.institutionCidade Universitária
dc.contributor.institutionSwedish Institute of Space Physics-IRF
dc.date.accessioned2025-04-29T19:34:30Z
dc.date.issued2023-11-01
dc.description.abstractContext. Chariklo has two narrow and dense rings, C1R and C2R, located at 391 km and 405 km, respectively. Aims. In the light of new stellar occultation data, we study the stability around Chariklo. We also analyse three confinement mechanisms that prevent the spreading of the rings, based on shepherd satellites in resonance with the edges of the rings. Methods. This study was performed through a set of numerical simulations and the Poincaré surface of section technique. Results. From the numerical simulation results, and from the current parameters referring to the shape of Chariklo, we verify that the inner edge of the stable region is much closer to Chariklo than the rings. The Poincaré surface of sections allows us to identify periodic and quasi-periodic orbits of the first kind, and also the resonant islands corresponding to the 1:2, 2:5, and 1:3 resonances. We construct a map of aeq versus eeq space that gives the location and width of the stable region and the 1:2, 2:5, and 1:3 resonances. Conclusions. We find that the first kind periodic orbit family can be responsible for a stable region whose location and size meet that of C1R, for specific values of the ring particle eccentricities. However, C2R is located in an unstable region if the width of the ring is assumed to be about 120 m. After analysing different systems, we propose that the best confinement mechanism is composed of three satellites: two satellites shepherding the inner edge of C1R and the outer edge of C2R, and the third satellite trapped in the 1:3 resonance.en
dc.description.affiliationGrupo de Dinâmica Orbital & Planetologia São Paulo State University-UNESP, Av. Ariberto Pereira da Cunha, 333
dc.description.affiliationUniversité de Paris Institut de Physique du Globe de Paris CNRS
dc.description.affiliationEldorado Research Institute Cidade Universitária, Av. Prof. Alan Turing 275
dc.description.affiliationSwedish Institute of Space Physics-IRF, Box 812
dc.description.affiliationUnespGrupo de Dinâmica Orbital & Planetologia São Paulo State University-UNESP, Av. Ariberto Pereira da Cunha, 333
dc.identifierhttp://dx.doi.org/10.1051/0004-6361/202345864
dc.identifier.citationAstronomy and Astrophysics, v. 679.
dc.identifier.doi10.1051/0004-6361/202345864
dc.identifier.issn1432-0746
dc.identifier.issn0004-6361
dc.identifier.scopus2-s2.0-85176726406
dc.identifier.urihttps://hdl.handle.net/11449/304298
dc.language.isoeng
dc.relation.ispartofAstronomy and Astrophysics
dc.sourceScopus
dc.subjectCelestial mechanics
dc.subjectMinor planets, asteroids: general
dc.subjectPlanets and satellites: rings
dc.titleThe stability around Chariklo and the confinement of its ringsen
dc.typeArtigopt
dspace.entity.typePublication
relation.isOrgUnitOfPublicationa4071986-4355-47c3-a5a3-bd4d1a966e4f
relation.isOrgUnitOfPublication.latestForDiscoverya4071986-4355-47c3-a5a3-bd4d1a966e4f
unesp.campusUniversidade Estadual Paulista (UNESP), Faculdade de Engenharia e Ciências, Guaratinguetápt

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