scholarly journals On the Quadratization of the Integrals for the Many-Body Problem

Mathematics ◽  
2021 ◽  
Vol 9 (24) ◽  
pp. 3208
Author(s):  
Yu Ying ◽  
Ali Baddour ◽  
Vladimir Gerdt ◽  
Mikhail Malykh ◽  
Leonid Sevastianov

A new approach to the construction of difference schemes of any order for the many-body problem that preserves all its algebraic integrals is proposed herein. We introduced additional variables, namely distances and reciprocal distances between bodies, and wrote down a system of differential equations with respect to the coordinates, velocities, and the additional variables. In this case, the system lost its Hamiltonian form, but all the classical integrals of motion of the many-body problem under consideration, as well as new integrals describing the relationship between the coordinates of the bodies and the additional variables are described by linear or quadratic polynomials in these new variables. Therefore, any symplectic Runge–Kutta scheme preserves these integrals exactly. The evidence for the proposed approach is given. To illustrate the theory, the results of numerical experiments for the three-body problem on a plane are presented with the choice of initial data corresponding to the motion of the bodies along a figure of eight (choreographic test).

1970 ◽  
Vol 141 (3) ◽  
pp. 620-630 ◽  
Author(s):  
W. Glöckle

1975 ◽  
Vol 69 ◽  
pp. 209-225 ◽  
Author(s):  
G. Contopoulos

The properties of conservative dynamical systems of two or more degrees of freedom are reviewed. The transition from integrable to ergodic systems is described. Nonintegrability is due to the interaction of two, or more, resonances. Then one sees, on a surface of section, infinite types of islands of various orders, while the asymptotic curves from unstable invariant points intersect each other along homoclinic and heteroclinic points producing an apparent ‘dissolution’ of the invariant curves. A threshold energy is defined separating near integrable systems from near ergodic ones. The possibility of real ergodicity for large enough energies is discussed. In the case of many degrees of freedom we also distinguish between integrable, ergodic, and intermediate cases. Among the latter are systems of particles interacting with Lennard-Jones interparticle potential. A threshold energy was derived, which is proportional to the number of particles. Finally some recent results about the general three-body problem are described. One can extend the families of periodic orbits of the restricted problem to the general three-body problem. Many of these orbits are stable. An empirical study of orbits near the stable periodic orbits indicates the existence of 2 integrals of motion besides the energy.


1956 ◽  
Vol 101 (3) ◽  
pp. 1186-1191 ◽  
Author(s):  
George J. Yevick ◽  
Jerome K. Percus
Keyword(s):  

2004 ◽  
Vol 30 (5) ◽  
pp. 349-356 ◽  
Author(s):  
V. V. Orlov ◽  
A. V. Petrova ◽  
A. V. Rubinov ◽  
A. I. Martynova

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