Secular resonance

Secular resonance

A secular resonance is a type of orbital resonance.

Secular resonances occur when the precession of two orbits is synchronised (a precession of the perihelion, of the ascending node, or both). A small body in secular resonance with a much larger one (e.g. a planet) will precess at the same rate as the large body. Over long times (a million years, or so) a secular resonance will change the eccentricity and inclination of the small body.

The effects of secular resonances are most studied in the context of the long-time evolution (millions of years or more) of minor planet orbits within the Asteroid belt.

One can distinguish
*"linear secular resonances" between a body and a single other large perturbing body (e.g. a planet), and
*"nonlinear secular resonances" involving more than one large body. [cite journal | author= V. Carruba et al| title= "On the V-type asteroids outside the Vesta family"| journal= Astronomy & Astrophysics| year= 2005| volume= 441| pages= 819]

ν6 resonance

A prominent example of a linear resonance is the "ν6 secular resonance" between asteroids and Saturn. Asteroids which approach it have their eccentricity slowly increased until they become mars-crossers, at which point they are usually ejected from the asteroid belt due to a close pass to Mars. This resonance forms the inner and "side" boundaries of the main asteroid belt around 2 AU, and at inclinations of about 20°.

References

ee also

*orbital resonance
*Asteroid belt


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