s. charnoz a. morbidelli

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Coupling the dynamical and collisional evolution of the Kuiper Belt, the Scattered Disk & the Oort Cloud S. Charnoz A. Morbidell i Equipe AIM Equipe AIM Université Paris 7 / CEA Saclay Université Paris 7 / CEA Saclay

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Coupling the dynamical and collisional evolution of the Kuiper Belt, the Scattered Disk & the Oort Cloud. S. Charnoz A. Morbidelli. Equipe AIM Université Paris 7 / CEA Saclay. A big mistery of the Kuiper Belt : The mass deficit. A popular scenario to explain the mass deficit is - PowerPoint PPT Presentation

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Page 1: S. Charnoz A. Morbidelli

Coupling the dynamical and collisional evolution of the Kuiper Belt, the Scattered Disk & the Oort Cloud

S. CharnozA. Morbidelli

Equipe AIMEquipe AIMUniversité Paris 7 / CEA SaclayUniversité Paris 7 / CEA Saclay

Page 2: S. Charnoz A. Morbidelli

A big mistery of the Kuiper Belt : The mass deficit

A popular scenario to explain the mass deficit isthe Collisional Griding of the KB over the age of the Solar System

We explore here some consequences of this scenario.

Page 3: S. Charnoz A. Morbidelli

Collisional Grinding Scenario

Start , dn/dr r-4.5

From Kenyon & Bromley 2004

end

Initial Conditions :

Steep size distribution +Only a few Plutos

Consequences :Strong erosion after 4 109 years.

Kenyon, Stern, Broomley, Weisman, Davis etc…

Page 4: S. Charnoz A. Morbidelli

3- In situe formation of the KBIn situe formation of the KB: Accretion + destruction occurs at the same place

The « recipe » of the today’s kuiper belt

2- KBO must have a very low material strength (~ 102 to 103 than usual estimates)

Kenyon & Luu, 1999

4- The system is described as a statistical set of particles at thermodynamical equilibrium(Particle in a Box) => Collisional griding occurs over the age of the Solar System=> Coarse description of the dynamics

1- The mass must be contained in small bodies that are naturally easy to break ( steep initial distrution (q~ -4.5) down to R~10m)

Page 5: S. Charnoz A. Morbidelli

BUT Other scenarios reproduce the KB size distribution : Dynamical depletion of the belt (see presentation by Morby)

=> Need very low collisonal evolution, initial SD= today’s SD

In short : All models seem to ~ reproduce the today’s size

distribution of the Kuiper Belt !!

How to be more discriminent ?

We should broaden the problem and take into account ….

Page 6: S. Charnoz A. Morbidelli

THE 4th ZONE !!

Page 7: S. Charnoz A. Morbidelli

From Dones et al. 2004

Broadening the problem : the Oort and the Scattered Disk

SD Objects KB

All 3 populations (KB, SD, OC) have their origin approximately in the same region

=> Similar StartingSize-distribution

Page 8: S. Charnoz A. Morbidelli

What are the consequences of the KB formation scenario for the evolution

Implication of steep-size distributions for the evolution of :

- Scattered Disk- Oort Cloud

The origin of the 3 populationscannot be studied separately

Page 9: S. Charnoz A. Morbidelli

IDEA: Test the collisional griding scenario for bodies of - Kuiper Belt- Oort Cloud - Scattered Disk

DIFFICULTY : To couple properly both the DYNAMICAL & COLLISIONALevolution of bodies: « Particle in a box » method cannot achieve this properly

ALGORITHM : Use of a new hybrid approach (Charnoz & Morbidelli Icarus 2004)that was used to compute evolution of bodies ejected by Jupiter and Saturn.

Page 10: S. Charnoz A. Morbidelli

Dynamical code : Integration of 6000 particles with J,S,U,N

Compute collision frequencies and velocities for all pairs of particles, with steps 104 years.

Each of 6000 particles holds a full size distributionevolved with a Fragmentation code :: Fragmentation + Craterisation

COUPLING DYNAMICAL with COLLISIONAL EVOLUTIONA Hybrid approach

Page 11: S. Charnoz A. Morbidelli

A REALISTIC DYNAMICALEVOLUTION

6000 independant size distributions evolved conjointlysame time

At the end of the Simulation~ 700 particles in the KB~ 10 particles in the SC~250 particles in the OC

Page 12: S. Charnoz A. Morbidelli

# 1 : The initial size distribution

is very steep, consistent with what is needed In the scenario : a few plutos, R_break~100m

Consistent with : Collisional griding scenarior

-4.5

-3.5Break Radius ~ 10m

# 2 : The initial size distribution is ~ today, but 100 times more massive

Consistent with : Dynamical depletion

r

NBreak Radius ~ 100 km

Investigation of 2 scenarios

Page 13: S. Charnoz A. Morbidelli

Evolution of the Kuiper Belt

Initial conditions : mass in small bodies Collisional grinding senario

Q=Benz &Asphaug 1999

CASE 1

Page 14: S. Charnoz A. Morbidelli

~ 20 times less massive than expected

=> As argued in Stern & Weissman (2001)

BUT big observational uncertainties exist for the Oort Cloud !!

Oort Cloud

Initial conditions : mass in small bodies

Collisional

grinding senario•From Flux of Long period cometsFrancis et al. 2005

« Observed* » : 4 1011 with D> 1km

Page 15: S. Charnoz A. Morbidelli

A too severe collisional evolution due to strong dynamical steeringof giant planets

Only ~ 107 bodies with D>1Km survive in the Scattered Disk.100 times less than Inferred from the observationof Jupiter Family comets(Duncan & Levison, 1997 )

Initial conditions : mass in small bodies

Collisional

grinding senario

Scattered Disk

*From flux of Jupiter family comets

Observed*: ~109 , D>1km

Trujjillo et al.2001~4x104, R>50 km

Page 16: S. Charnoz A. Morbidelli

CASE 2

The Oort Cloud

« Observed* » : 4 1011 with D> 1km

Much better machWith the estimated populationOf the Oort Cloud

Page 17: S. Charnoz A. Morbidelli

The Scattered Disk

Trujjillo et al.2001~4x104, R>50 km

Observed*: ~109 , D>1km

Good match toobservartions

Page 18: S. Charnoz A. Morbidelli

The Kuiper Belt

Good shape of the S.D.

But to get the right (low) mass onlythe scenario of dynamicalImplantation seem to work

Page 19: S. Charnoz A. Morbidelli

SUMMARY-Using a new and hybrid approach to couple collisional and dynamical evolution, we show that :

3- Dynamical depletion, not collisional erosion, should be responsible for the mass deficit of the KB

2- The collisional griding of the KB has severe problems :

- The Oort Cloud is too severly depleted by a factor of ~ 20- The Scattered Disk is too severely depleted by a factor of 100

1- In every scenario, the most severly depleted population is the SCATTERED DISK

Charnoz & Morbidelli 2007, ICARUS In press Reprints : [email protected]

Page 20: S. Charnoz A. Morbidelli

SUGGESTIONS FOR NEW HORIZONS

- Observation of the surface moderately big objects (>50 and < 200 km) Kuiper Belt objects may help to determine the Cratering rate and the constrain the flux of impactors over the age of the Solar System

-Observation of small (<10 km) Kuiper belt objects may help detrmine if they arePristine or not (difficult !!) . * scattered disk bodies are better here*

Such data may be critical to better constrain the formation scenario of the KB Region and may help to decide which « story » is the right one :Collisional erosion ? Dynamical Depletion ?

(A. Stern may have a preference for the first !!)

Page 21: S. Charnoz A. Morbidelli

THE END

Page 22: S. Charnoz A. Morbidelli

The Oort Cloud population

Divided into 2 parts :

The « visible » or Outer Oort Cloud with a> 104 au

The Inner Oort Cloudwith a<104 au

Total : ~ 4 1011 bodies with D>1km

Page 23: S. Charnoz A. Morbidelli

CLEAR OPPOSITION BETWEEN 2 MODELS OF KUIPER BELT ORIGIN

Collisional Griding Dynamical erosion

Mass in small bodies

Steep S.D.

A few plutos

Mass in big bodies

shallow S.D.

A few 100 plutos

N

r

-4.5

-3.5Break Radius ~ 10m

r

NBreak Radius ~ 100 km

?How to get out of the dilemna ?

Page 24: S. Charnoz A. Morbidelli

Other Scenario : mass in big bodies Dynamical depletion

The size distribution almost does not evolve under collisions

Reasonable results forOort Cloud (4 time less)Scattered Disk (OK)

Page 25: S. Charnoz A. Morbidelli

The outer edge of the Solar System is occupied by 3 populationsof small bodies whose dynamical & collisional history is coupled

1. The Kuiper Belt

~ 0.01-0.1 Me

2. The Scattered disk

~ 109 with D> 1km

Gladman et al. 2005

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