{"title":"二维动力系统不变流形的吸引性","authors":"Pei Lijun","doi":"10.1109/IWCFTA.2012.15","DOIUrl":null,"url":null,"abstract":"In this paper an operable, universal and simple theory on the attractiveness of the invariant manifolds of the two-dimensional dynamical systems is first obtained. It is motivated by the Lyapunovdirect method. It means that for any point x<sup>→</sup> in the invariant manifold M, n(x<sup>→</sup>) is the normal passing by x<sup>→</sup>, and ∀x<sup>→</sup> ∈n(x<sup>→</sup>), if the tangent f(x<sup>→</sup>) of the orbit of the dynamical system intersects at obtuse (sharp) angle with the n(x<sup>→</sup>), or the inner product of the normal vector n<sup>→</sup>(x<sup>→</sup>) and tangent vector f<sup>→</sup>(x<sup>→</sup>) is negative (positive), i.e., f<sup>→</sup>(x<sup>→</sup>). n<sup>→</sup>(x<sup>→</sup>) <; (>;)0, then the invariant manifold M is attractive (repulsive). Some illustrative examples of the invariant manifolds, such as equilibria, periodic solution, stable and unstable manifolds, other invariant manifold are presented to support this result.","PeriodicalId":354870,"journal":{"name":"2012 Fifth International Workshop on Chaos-fractals Theories and Applications","volume":"12 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2012-10-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Attractiveness of Invariant Manifolds of Two Dimensional Dynamical Systems\",\"authors\":\"Pei Lijun\",\"doi\":\"10.1109/IWCFTA.2012.15\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this paper an operable, universal and simple theory on the attractiveness of the invariant manifolds of the two-dimensional dynamical systems is first obtained. It is motivated by the Lyapunovdirect method. It means that for any point x<sup>→</sup> in the invariant manifold M, n(x<sup>→</sup>) is the normal passing by x<sup>→</sup>, and ∀x<sup>→</sup> ∈n(x<sup>→</sup>), if the tangent f(x<sup>→</sup>) of the orbit of the dynamical system intersects at obtuse (sharp) angle with the n(x<sup>→</sup>), or the inner product of the normal vector n<sup>→</sup>(x<sup>→</sup>) and tangent vector f<sup>→</sup>(x<sup>→</sup>) is negative (positive), i.e., f<sup>→</sup>(x<sup>→</sup>). n<sup>→</sup>(x<sup>→</sup>) <; (>;)0, then the invariant manifold M is attractive (repulsive). Some illustrative examples of the invariant manifolds, such as equilibria, periodic solution, stable and unstable manifolds, other invariant manifold are presented to support this result.\",\"PeriodicalId\":354870,\"journal\":{\"name\":\"2012 Fifth International Workshop on Chaos-fractals Theories and Applications\",\"volume\":\"12 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2012-10-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2012 Fifth International Workshop on Chaos-fractals Theories and Applications\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/IWCFTA.2012.15\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2012 Fifth International Workshop on Chaos-fractals Theories and Applications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IWCFTA.2012.15","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Attractiveness of Invariant Manifolds of Two Dimensional Dynamical Systems
In this paper an operable, universal and simple theory on the attractiveness of the invariant manifolds of the two-dimensional dynamical systems is first obtained. It is motivated by the Lyapunovdirect method. It means that for any point x→ in the invariant manifold M, n(x→) is the normal passing by x→, and ∀x→ ∈n(x→), if the tangent f(x→) of the orbit of the dynamical system intersects at obtuse (sharp) angle with the n(x→), or the inner product of the normal vector n→(x→) and tangent vector f→(x→) is negative (positive), i.e., f→(x→). n→(x→) <; (>;)0, then the invariant manifold M is attractive (repulsive). Some illustrative examples of the invariant manifolds, such as equilibria, periodic solution, stable and unstable manifolds, other invariant manifold are presented to support this result.