@Article{AraujoWintPradSukh:2012:StReAr,
author = "Araujo, R. A. N. and Winter, Othon Cabo and Prado, Antonio
Fernando Bertachini de Almeida and Sukhanov, A.",
affiliation = "UNESP - S{\~a}o Paulo State University, CEP 12516-410
Guaratinguet{\'a}, SP, Brazil and UNESP - S{\~a}o Paulo State
University, CEP 12516-410 Guaratinguet{\'a}, SP, Brazil and
{Instituto Nacional de Pesquisas Espaciais (INPE)}",
title = "Stability regions around the components of the triple system 2001
SN263",
journal = "Monthly Notices of the Royal Astronomical Society",
year = "2012",
volume = "423",
number = "4",
pages = "3058--3073",
month = "July",
keywords = "celestial mechanics, N-body simulations, minor planets, asteroids,
astrodin{\^a}mica, manobras orbitais, trajet{\'o}rias
espaciais.",
abstract = "Space missions are an excellent way to increase our knowledge of
asteroids. Near-Earth asteroids (NEAs) are good targets for such
missions, as they periodically approach the orbit of the Earth.
Thus, an increasing number of missions to NEAs are being planned
worldwide. Recently, NEA (153591) 2001 SN263 was chosen as the
target of the ASTER MISSION - the First Brazilian Deep Space
Mission, with launch planned for 2015. NEA (153591) 2001 SN263 was
discovered in 2001. In 2008 February, radio astronomers from
Arecibo-Puerto Rico concluded that (153591) 2001 SN263 is actually
a triple system. The announcement of ASTER MISSION has motivated
the development of the present work, whose goal is to characterize
regions of stability and instability of the triple system (153591)
2001 SN263. Understanding and characterizing the stability of such
a system is an important component in the design of the mission
aiming to explore it. The method adopted consisted of dividing the
region around the system into four distinct regions (three of them
internal to the system and one external). We performed numerical
integrations of systems composed of seven bodies, namely the Sun,
Earth, Mars, Jupiter and the three components of the asteroid
system (Alpha, the most massive body; Beta the second most massive
body; and Gamma, the least massive body), and of thousands of
particles randomly distributed within the demarcated regions, for
the planar and inclined prograde cases. The results are displayed
as diagrams of semi-major axis versus eccentricity that show the
percentage of particles that survive for each set of initial
conditions. The regions where 100per cent of the particles survive
are defined as stable regions. We found that the stable regions
are in the neighbourhood of Alpha and Beta, and in the external
region. Resonant motion of the particles with Beta and Gamma was
identified in the internal regions, leading to instability. For
particles with I > 45° in the internal region, where I is the
inclination with respect to Alpha's equator, there is no stable
region, except for particles placed very close to Alpha. The
stability in the external region is not affected by the variation
of inclination. We also present a discussion of the long-term
stability in the internal region, for the planar and circular
case, with comparisons with the short-term stability.",
doi = "10.1111/j.1365-2966.2012.21101.x",
url = "http://dx.doi.org/10.1111/j.1365-2966.2012.21101.x",
issn = "1365-2966",
label = "lattes: 7340081273816424 3 AraujoWintPradSukh:2012:StReAr",
language = "en",
targetfile = "Stability regions around the components.pdf",
urlaccessdate = "30 abr. 2024"
}