The perturbed three-dimensional two body problem: regular quaternion equations of relative motion

2018 ◽  
Vol 82 (6) ◽  
pp. 721-733
Author(s):  
Yu. Chelnokov ◽  
1973 ◽  
pp. 69-109 ◽  
Author(s):  
V. G. Kadyshevskii ◽  
R. M. Mir-Kasimov ◽  
N. B. Skachkov

1977 ◽  
Vol 30 (3) ◽  
pp. 212-221 ◽  
Author(s):  
I. V. Amirkhanov ◽  
G. V. Grusha ◽  
R. M. Mir-Kasimov

2001 ◽  
Vol 12 (05) ◽  
pp. 739-750 ◽  
Author(s):  
I. N. NIKITIN ◽  
J. DE LUCA

We develop two numerical methods to solve the differential equations with deviating arguments for the motion of two charges in the action-at-a-distance electrodynamics. Our first method uses Stürmer's extrapolation formula and assumes that a step of integration can be taken as a step of light ladder, which limits its use to shallow energies. The second method is an improvement of pre-existing iterative schemes, designed for stronger convergence and can be used at high-energies.


Author(s):  
Nathalie Deruelle ◽  
Jean-Philippe Uzan

This chapter embarks on a study of the two-body problem in general relativity. In other words, it seeks to describe the motion of two compact, self-gravitating bodies which are far-separated and moving slowly. It limits the discussion to corrections proportional to v2 ~ m/R, the so-called post-Newtonian or 1PN corrections to Newton’s universal law of attraction. The chapter first examines the gravitational field, that is, the metric, created by the two bodies. It then derives the equations of motion, and finally the actual motion, that is, the post-Keplerian trajectories, which generalize the post-Keplerian geodesics obtained earlier in the chapter.


Author(s):  
Nathalie Deruelle ◽  
Jean-Philippe Uzan

This chapter presents the basics of the ‘effective-one-body’ approach to the two-body problem in general relativity. It also shows that the 2PN equations of motion can be mapped. This can be done by means of an appropriate canonical transformation, to a geodesic motion in a static, spherically symmetric spacetime, thus considerably simplifying the dynamics. Then, including the 2.5PN radiation reaction force in the (resummed) equations of motion, this chapter provides the waveform during the inspiral, merger, and ringdown phases of the coalescence of two non-spinning black holes into a final Kerr black hole. The chapter also comments on the current developments of this approach, which is instrumental in building the libraries of waveform templates that are needed to analyze the data collected by the current gravitational wave detectors.


Sign in / Sign up

Export Citation Format

Share Document