scholarly journals Poincaré surfaces of section around a 3D irregular body: the case of asteroid 4179 Toutatis

2017 ◽  
Vol 474 (2) ◽  
pp. 2452-2466 ◽  
Author(s):  
G Borderes-Motta ◽  
O C Winter
PLoS ONE ◽  
2017 ◽  
Vol 12 (12) ◽  
pp. e0187798 ◽  
Author(s):  
Markus Guerster ◽  
Ulrich Walter
Keyword(s):  

Author(s):  
Sarah Morrison ◽  
Doug Hemingway
Keyword(s):  

2015 ◽  
Vol 2015 ◽  
pp. 1-11 ◽  
Author(s):  
Flaviane C. F. Venditti ◽  
Antonio F. B. A. Prado

The orbital dynamics around irregular shaped bodies is an actual topic in astrodynamics, because celestial bodies are not perfect spheres. When it comes to small celestial bodies, like asteroids and comets, it is even more import to consider the nonspherical shape. The gravitational field around them may generate trajectories that are different from Keplerian orbits. Modeling an irregular body can be a hard task, especially because it is difficult to know the exact shape when observing it from the Earth, due to their small sizes and long distances. Some asteroids have been observed, but it is still a small amount compared to all existing asteroids in the Solar System. An approximation of their shape can be made as a sum of several known geometric shapes. Some three-dimensional figures have closed equations for the potential and, in this work, the formulation of a cube is considered. The results give the mappings showing the orbits that are less perturbed and then have a good potential to be used by spacecrafts that need to minimize station-keeping maneuvers. Points in the orbit that minimizes the perturbations are found and they can be used for constellations of nanosatellites.


Author(s):  
Sarah Morrison ◽  
Doug Hemingway
Keyword(s):  

2019 ◽  
Vol 7 (2) ◽  
pp. 49
Author(s):  
Abdullah A. Ansari ◽  
Ashraf Ali ◽  
Kumari Shalini ◽  
Mehtab Alam

This paper investigates the motion of the massless body moving under the influence of the gravitational forces of the three equal heterogeneous oblate spheroids placed at Lagrangian configuration. After determining the equations of motion and the Jacobian constant of the massless body, we have illustrated the numerical work (Stationary points, zero-velocity curves, regions of motion, Poincare surfaces of section and basins of attraction). And then we have checked the linear stability of the stationary points and found that all the stationary points are unstable. 


1993 ◽  
Vol 48 (4) ◽  
pp. 584-594
Author(s):  
Georg R. Siegert ◽  
Roland G. Winkler ◽  
Peter Reineker

Abstract The dynamics of a short freely jointed chain of three segments is investigated numerically. The chain consists of mass points connected by massless rigid rods, its initial and final points being fixed. Thus the chain represents a holonomically constrained system with three degrees of freedom. It is shown that the motion of the mass points can be chaotic; the occurrence of chaos depends on the initial conditions of the motion, the end-to-end distance of the chain, and the angular momentum about the axis of the stretching direction. Moreover, the chain more likely exhibits regular than chaotic behavior. The numerical results are presented in the form of Poincare surfaces of section, including the use of a slice technique, as well as in the form of power spectra.


Author(s):  
Xulong YUAN ◽  
Xiyan LIU ◽  
Cheng CHEN ◽  
Yao REN ◽  
Biancheng ZHANG

1994 ◽  
Vol 04 (06) ◽  
pp. 1535-1562 ◽  
Author(s):  
HOLGER R. DULLIN ◽  
MARCUS JUHNKE ◽  
PETER H. RICHTER

The different types of energy surfaces are identified for the Kovalevskaya problem of rigid body dynamics, on the basis of a bifurcation analysis of Poincaré surfaces of section. The organization of their foliation by invariant tori is qualitatively described in terms of Poincaré-Fomenko stacks. The individual tori are then analyzed for sets of independent closed paths, using a new algorithm based on Arnold’s proof of the Liouville theorem. Once these paths are found, the action integrals can be calculated. Energy surfaces are constructed in the space of action variables, for six characteristic values of energy. The data are presented in terms of color graphs that give an intuitive access to this highly complex integrable system.


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