The famous three-body problem can be traced back to Isaac Newton in the 1680s. In the 300 years since this “three-body problem” was first recognized, only three families of periodic solutions had been found, until 2013 when Šuvakov and Dmitrašinović [Phys. Rev. Lett. 110, 114301 (2013)] made a breakthrough to numerically find 13 new distinct periodic orbits, which belong to 11 new families of Newtonian planar three-body problem with equal mass and zero angular momentum. In this paper, we numerically obtain 695 families of Newtonian periodic planar collisionless orbits of three-body system with equal mass and zero angular momentum in case of initial conditions with isosceles collinear configuration, including the well-known figure-eight family found by Moore in 1993, the 11 families found by Šuvakov and Dmitrašinović in 2013, and more than 600 new families that have never been reported, to the best of our knowledge. With the definition of the average period T = T/Lf, where Lf is the length of the so-called “free group element”, these 695 families suggest that there should exist the quasi Kepler’s third law T* ≈ 2:433 ± 0:075 for the considered case, where T ≈ = T |E|3/2 is the scale-invariant average period and E is its total kinetic and potential energy, respectively. The movies of these 695 periodic orbits in the real space and the corresponding close curves on the “shape sphere” can be found via the website: http://numericaltank.sjtu.edu.cn/three-body/three-body.htm.
three-body problem periodic orbits clean numerical simulation (CNS)
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This work was partly supported by the National Natural Science Foundation of China (Grant No. 11432009). This work was carried out on TH-2 at National Supercomputer Centre in Guangzhou, China.
D. Rose, Geometric Phase and Periodic Orbits of the Equalmass, Planar Three-body Problem with Vanishing Angular Momentum, Dissertation for Doctoral Degree (University of Sydney, Sydney, 2016).Google Scholar