22.01.2014 Views

Techniques d'observation spectroscopique d'astéroïdes

Techniques d'observation spectroscopique d'astéroïdes

Techniques d'observation spectroscopique d'astéroïdes

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

CHAPTER 1. WHY ASTEROIDS? 37<br />

tel-00785991, version 1 - 7 Feb 2013<br />

Owing to some mechanisms some of the Main Belt Asteroids have migrated into the inner<br />

part of the Solar System [Morbidelli et al., 2002]. These are Near-Earth Asteroids (denoted<br />

NEAs), small bodies of the Solar System with perihelion distances q ≤ 1.3 AU and aphelion<br />

distances Q≥0.983AU, whose orbits approach or intersect Earth orbit. Dynamical studies confirmed<br />

the main belt origin for the majority of NEAs population. The transition of a main belt<br />

asteroid to NEA class is due to the dynamical perturbations associated with the main belt resonances.<br />

The most active of these regions acting as escape hatches are the ν6 secular resonance<br />

and the orbital resonances 3:1, 5:2 and 2:1 with Jupiter situated at 2.5, 2.8 et 3.2 astronomical<br />

units. Long term numerical integrations have revealed the source regions of the current NEAs<br />

population: 61% originated in the inner region of main belt, 24% in the central and 8% in the<br />

outer main belt. Only 6% of NEAs are considered to have a cometary origin. The steady-state<br />

model of NEA will require a constant flux of objects with H≤18 of 800/Myr.<br />

Depending on their orbital parameters, NEAs are subdivided into Amors (1.016 < q < 1.3<br />

AU), Apollos (a ≥ 1.0 AU; q ≤ 1.016 AU), Athens (semi-major axe a < 1.0 AU; Q ≥ 0.983<br />

AU), and Atiras (Q

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!