SearcharxivSearch

arXiv · chao-dyn/9709022

Dynamical Instability and Statistical Behaviour of N-Body Systems

Abstract

We here describe the possibility of a synthetic description of the onset of Chaos in many degrees of freedom dynamical systems within the framework of the geometric description of dynamics. We show how this approach to instability helps to single out the transition between different regimes of stochasticity in typical as well peculiar N-body systems. It is shown how intermingled are the relationships between geometric properties of the manifold and stability properties of the dynamics, which do not follow any naive prescription. The implications concerning the possibility of a Statistical description are also addressed, and it is shown how the peculiarities of the interaction potential reflect themselves also on the geometric description. In particular, it is found that for the gravitational N-body system the dynamics possess features very similar to those of stable and tempered many body dynamical systems in the regime of strong stochasticity. All these issues are addressed from a semi-analytical approach, checked using well tailored numerical simulations, which help also to reinterpret some results recently appeared, and to correct to some extent previous claims presented in the literature.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Cipriani Piero, Di Bari Maria. 1997-09-18. Dynamical Instability and Statistical Behaviour of N-Body Systems. https://arxiv.org/abs/chao-dyn/9709022

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

The Bogdanov Map: Bifurcations, Mode Locking, and Chaos in a Dissipative System

We investigate the bifurcations and basins of attraction in the Bogdanov map, a planar quadratic map which is conjugate to the Hénon area-preserving map in its conservative limit. It undergoes a Hopf bifurcation as dissipation is added, and exhibits the panoply of mode locking, Arnold tongues, and chaos as an invariant circle grows out, finally to be destroyed in the homoclinic tangency of the manifolds of a remote saddle point. The Bogdanov map is the Euler map of a two-dimensional system of ordinary differential equations first considered by Bogdanov and Arnold in their study of the versal unfolding of the double-zero-eigenvalue singularity, and equivalently of a vector field invariant under rotation of the plane by an angle $2π$. It is a useful system in which to observe the effect of dissipative perturbations on Hamiltonian structure. In addition, we argue that the Bogdanov map provides a good approximation to the dynamics of the Poincaré maps of periodically forced oscillators.

chao-dyn

Passive Scalars and Three-Dimensional Liouvillian Maps

Global aspects of the motion of passive scalars in time-dependent incompressible fluid flows are well described by volume-preserving (Liouvillian) three-dimensional maps. In this paper the possible invariant structures in Liouvillian maps and the two most interesting nearly-integrable cases are investigated. In addition, the fundamental role of invariant lines in organizing the dynamics of this type of system is exposed. Bifurcations involving the destruction of some invariant lines and tubes and the creation of new ones are described in detail.

chao-dyn