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Using a completely analytic procedure - based on a suitable extension of a classical method - we discuss an approach to the Poincar\'e-Mel'nikov theory, which can be conveniently applied also to the case of non-hyperbolic critical points,…

chao-dyn · Physics 2009-10-31 G. Cicogna , M. Santoprete

We prove the existence of chaotic trajectories for the two body problem on a sphere. The trajectories we construct encounter near-collisions and are similar to the second species solutions of Poincar\'e of the classical 3 body problem. The…

Dynamical Systems · Mathematics 2025-11-25 Sergey Bolotin

Three types of orbits are theoretically possible in autonomous Hamiltonian systems with three degrees of freedom: fully chaotic (they only obey the energy integral), partially chaotic (they obey an additional isolating integral besides…

Astrophysics of Galaxies · Physics 2017-08-30 J. C. Muzzio

Homoclinic chaos is usually examined with the hypothesis of hyperbolicity of the critical point. We consider here, following a (suitably adjusted) classical analytic method, the case of non-hyperbolic points and show that, under a…

chao-dyn · Physics 2009-10-31 G. Cicogna , M. Santoprete

We study the dynamics of the planar circular restricted three-body problem in the context of a pseudo-Newtonian approximation. By using the Fodor-Hoenselaers-Perj\'es procedure, we perform an expansion in the mass potential of a static…

General Relativity and Quantum Cosmology · Physics 2017-01-05 F. L. Dubeibe , F. D. Lora-Clavijo , Guillermo A. González

We study the equal-mass classical three rotor problem, a variant of the three body problem of celestial mechanics. The quantum $N$-rotor problem has been used to model chains of coupled Josephson junctions and also arises via a partial…

Chaotic Dynamics · Physics 2019-09-25 Govind S. Krishnaswami , Himalaya Senapati

We use a third-order perturbation theory and Melnikov's method to prove the existence of chaos in spinning circular disks subject to a lateral point load. We show that the emergence of transverse homoclinic and heteroclinic points…

Chaotic Dynamics · Physics 2009-11-13 Arzhang Angoshtari , Mir Abbas Jalali

This paper concerns the classical dynamics of three coupled rotors: equal masses moving on a circle subject to attractive cosine inter-particle potentials. It is a simpler variant of the gravitational three-body problem and also arises as…

Chaotic Dynamics · Physics 2019-12-24 Govind S. Krishnaswami , Himalaya Senapati

The description of unstable motions in the Restricted Planar Circular 3-Body Problem, modeling the dynamics of a Sun-Planet-Asteriod system, is one of the fundamental problems in Celestial Mechanics. The goal of this paper is to analyze…

Dynamical Systems · Mathematics 2023-12-22 Inmaculada Baldomá , Mar Giralt , Marcel Guardia

The Sitnikov problem is a special case of the three-body problem. The system is known to be chaotic and has been studied by symbolic dynamics (J. Moser, Stable and random motions in dynamical systems, Princeton University Press, 1973). We…

Dynamical Systems · Mathematics 2025-08-12 Yuika Kajihara , Mitsuru Shibayama , Guowei Yu

This thesis studies instabilities and singularities in a geometrical approach to the planar 3-body problem as well as instabilities, chaos and ergodicity in the 3-rotor problem. Trajectories of the planar 3-body problem are expressed as…

Chaotic Dynamics · Physics 2020-08-07 Himalaya Senapati

In a system of particles, quasi-periodic almost-collision orbits are collisionless orbits along which two bodies become arbitrarily close to each other -- the lower limit of their distance is zero but the upper limit is strictly positive --…

Dynamical Systems · Mathematics 2013-08-13 Lei Zhao

In this work the Melnikov method for perturbed Hamiltonian wave equations is considered in order to determine possible chaotic behaviour in the systems. The backbone of the analysis is the multi-symplectic formulation of the unperturbed PDE…

Chaotic Dynamics · Physics 2007-05-23 K. B. Blyuss

We consider the 3-body problem in relativistic lineal gravity and obtain an exact expression for its Hamiltonian and equations of motion. While general-relativistic effects yield more tightly-bound orbits of higher frequency compared to…

General Relativity and Quantum Cosmology · Physics 2009-11-07 F. J. Burnell , R. B. Mann , T. Ohta

In this paper we research global dynamics and bifurcations of planar piecewise smooth quadratic quasi--homogeneous but non-homogeneous polynomial differential systems. We present sufficient and necessary conditions for the existence of a…

Dynamical Systems · Mathematics 2017-08-14 Yilei Tang

We have investigated the appearance of chaos in the 1-dimensional Newtonian gravitational three-body system (three masses on a line with $-1/r$ pairwise potential). We have concentrated in particular on how the behavior changes when the…

chao-dyn · Physics 2009-10-22 Jarmo Hietarinta , Seppo Mikkola

The discovery of Pluto's small moons in the last decade brought attention to the dynamics of the dwarf planet's satellites. With such systems in mind, we study a planar $N$-body system in which all the bodies are point masses, except for a…

Earth and Planetary Astrophysics · Physics 2018-07-04 James A. Kwiecinski , Attila Kovacs , Andrew L. Krause , Ferran Brosa Planella , Robert A. Van Gorder

We consider the planar circular restricted three-body problem (PCRTBP), as a model for the motion of a spacecraft relative to the Earth-Moon system. We focus on the Lagrange equilibrium points $L_1$ and $L_2$. There are families of Lyapunov…

Dynamical Systems · Mathematics 2022-01-12 Marian Gidea , Rafael de la Llave , Maxwell Musser

Periodicity plays a significant role in the chaos theory from the beginning since the skeleton of chaos can consist of infinitely many unstable periodic motions. This is true for chaos in the sense of Devaney [1], Li-Yorke [2] and the one…

Chaotic Dynamics · Physics 2017-04-25 Marat Akhmet , Mehmet Onur Fen

We consider a $2$-dimensional autonomous system subject to a $1$-periodic perturbation, i.e. $$ \dot{\vec{x}}=\vec{f}(\vec{x})+\epsilon\vec{g}(t,\vec{x},\epsilon),\quad \vec{x}\in\Omega .$$ We assume that for $\epsilon=0$ there is a…

Dynamical Systems · Mathematics 2025-09-11 Alessandro Calamai , Matteo Franca , Michal Pospisil
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