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(1)

Dynamics and Impact Monitoring

(2)

 Dynamics of asteroids

• Impact monitoring

• Orbit resonances

• Deflection

 Evolving risk assessment: how does the uncertainty for the hazardous

impact objects evolve with time?

 How can dynamics finding be used for astronomical orbit

determinations?

(3)

 Öpik’s theory for close encounters (extended to include near misses,

Valsecchi, et al., 2003)

 The b-plane allows to conveniently

characterise an encounter, as it decouples its two main parameters

 b-plane coordinates

• 𝜉 represents the geometric distance between the orbits

• 𝜁 represents the shift in arrival time of the object at the planet

 The impact parameter is defined as

𝑏 = 𝜉2 + 𝜁2

Dynamics and impact monitoring

Resonant encounters

(4)

 In order to have a subsequent

planetary encounter of the object, the following condition must be

satisfied: 𝑘Τ𝑃 = ℎΤ′, 𝑘, ℎ ∈ ℕ

 The normalised post-encounter

semi-major axis can be defined as

𝑎′ = 𝑘 2 3

 This parameter is associated to

the post-encounter Θ angle

 The combination of this result

with the description of the angles after the flyby gives the equation of a circle on the b-plane centred on the 𝜁 axis in 𝐷, with a radius 𝑅

Dynamics and impact monitoring

Resonant encounters

(5)

Dynamics and impact monitoring

Example of resonant dynamicsAriane launcher of BepiColombo

 Letizia F., Van den Eynde J., Colombo C., Jehn R., “Evaluation of

Compliance to Planetary Protection Requirements with SNAPPshot.”, Submitted to Advances in Space Research, 2018.

(6)

 The maximisation of 𝑑𝜉 is the only non-cumulative effect and the

only one to present a periodic behaviour

 The maximisation of 𝑑𝜁 is

therefore considerably more effective than that of 𝑑𝜉, thus closely resembling that of 𝑑𝑏 for long deviation times

Dynamics and impact monitoring

Optimal deflection missions

(7)

Propagation for 100

years after the deviation to observe the following close approaches on the b-plane

Dynamics and impact monitoring

Deflection of resonant encounters

Example of post-deviation b-plane analysis for 2010 RF12, only the first close approach is visible, as the others are far from the centre

(8)

 Dynamics of orbits around NEOs

• Specific to in situ studies

• Specific to deflections

• Manipulation

 What kind of orbits can we use for future missions?

 Sinergy between capture and deflection?

(9)

Rotating Hill frame A centred at the asteroid

Dynamics and impact monitoring

Dynamics at asteroids

Maximum velocity on the axis of maximum inertia

Riferimenti

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