+ All Categories
Home > Documents > The Kuiper Belt as a Debris Disk - Lunar and Planetary …renu/malhotra_preprints/04-TPF... ·  ·...

The Kuiper Belt as a Debris Disk - Lunar and Planetary …renu/malhotra_preprints/04-TPF... ·  ·...

Date post: 15-Apr-2018
Category:
Upload: lytu
View: 215 times
Download: 0 times
Share this document with a friend
17
The Kuiper Belt as a Debris Disk Renu Malhotra University of Arizona a vast swarm of small bodies orbiting just beyond Neptune Art by Don Dixon (2000) 1
Transcript

The Kuiper Belt as a Debris Disk

Renu MalhotraUniversity of Arizona

a vast swarm of small bodies orbiting just beyond NeptuneArt by Don Dixon (2000)

1

Dynamical classes

Multi-opposition TNOs+SDOs+Centaurs: orbital distribution

(data from MPC/05-july-2004)

0

0.2

0.4

5:33:2 2:1

30 35 40 45 50 550

10

20

30

40

a (AU)

• Resonant KBOs(e.g., 3:2, 2:1, 5:2)

• Main Belt (40 . a . 47 AU,ie, between 3:2 and 2:1)

• Scattered Disk(a > 50 AU & 30 < q . 36 AU)

– Extended Scattered Disk(a� 50 AU & q & 36 AU)

• Centaurs (q < aNeptune)

2

The Hot and Cold Main BeltMulti-opposition TNOs+SDOs+Centaurs: orbital distribution

(data from MPC/05-july-2004)

0

0.2

0.4

5:33:2 2:1

30 35 40 45 50 550

10

20

30

40

a (AU)

3

The Extended Scattered DiskMulti-opposition TNOs+SDOs+Centaurs: orbital distribution

(data from MPC/05-july-2004)

0

0.2

0.4

0.6

0.8

100 200 300 400 5000

10

20

30

40

a (AU)

4

The Edge of the Main Belt(Allen, Bernstein & Malhotra 2001, Trujillo & Brown 2001)

KB Radial distribution (Trujillo & Brown, 2001). 5

Size Distribution

Bernstein et al (2004).(Red =“Classical disk”= i≤5◦ and 38<d<55 AU;

Green =“Excited” class = complement of “classical”)

• Observed KBOs have radii10.R.1000 km– N(R > 50 km) � 5� 104

– main belt mass� 0:01 M⊕– total mass (<50AU) . 0:03M⊕– � 100� asteroid belt

• Size-class correlations– “excited” KBOs contain more large

objects & fewer small objects comparedto the “classical” KBOs

– largest CKBO is 1/60th mass of Pluto

• Collisional evolution models (Stern1995, Durda & Stern 2000) indicate thatcollisions are destructive for D . 100–300km, in the present environment

• The source of short period Jupiter-familycomets (JFCs): Uncertain. The scattereddisk may be the more likely source...

• Accretion models (Stern 1995, Kenyon & Luu 1999) indicate that R & 50 km KBOs must haveformed in a dynamically cold environment, ie, (e, i)initial . 0.001

– Some process has disturbed the Kuiper Belt & pumped up KBOs’ e’s and i’s6

Resonant Kuiper Belt Objects

-55 -50 -45 -40 -35 -30

-1

0

1

X (AU)

-40 -20 0 20 40

-40

-20

0

20

40

X/AU

J S U N

P

Pluto’s 3:2 mean motion resonance with Neptune

0 0.2 0.4 0.6 0.8 10

100

200

300

time (Gyr)

47

47.5

48

48.5

49

0

0.05

0.1

0.15

0.2

0

5

10

A weakly chaotic twotino

7

Resonance sweeping by a migrating Neptune

Neptune Pluto/Plutino

Sun

30 AU 2/13/2

0

50

100

1503:2

2:1

5:3

8

Why would the giant planets migrate?

from Hahn & Malhotra (1999)

• cores of giant planets formedwithin a planetesimal disk

• planet–formation was likely not100% efficient

– residual planetesimal debris isleft over

• recently–formed planets scatterthe planetesimal debris, exchangeL with planetesimal disk

• Nbody simulations (Fernandez & Ip1984, Hahn & Malhotra 1999, Gomes,Morby, Levison 2004) show planetsevolve away from each other, ie,Jupiter inwards, Neptune outwards

9

How far did Neptune migrate?• Neptune’s outward migration

causes its mean motionresonances (MMR’s) to sweepout across the Kuiper Belt

• KBOs get trapped at MMR’s,are dragged outwards,and have their e pumped up

• Malhotra (1993) showed thismechanism can account forPluto’s orbit (in 3:2 with e = 0.25,∆a ≈ 5 AU)

• The e-pumping depends uponNeptune’s ∆a

• A particle trapped at a j + k : j MMR has an adiabatic invariant,

B = a(√

1− e2 − jj+k)

2 ⇒ e(a)2 = 1−(

j+k√

ainitial/aj+k

)2

if einit = 0

• Plutinos (j = 2,k = 1) have emax = 0.33, so they were dragged fromainitial = 27.3 to a = 39.5 AU, i.e., ∆a ≈ 12 AU– hence, Neptune migrated ∆aNep = ∆a/(3/2)2/3 ≈ 9 AU

10

SIMULATION OF ADIABATIC RESONANCE SWEEPING OF THE KUIPER BELT(from Malhotra, 1995)

0

0.1

0.2

0.3

0.4

0

10

20

30 35 40 45 500

50

100

150

a (AU)

3:24:3 5:3 2:1

Challenges

• Twotino population is too small– chaotic diffusion over 4 Gyr =⇒ p. 12

• Observed inclinations are difficult to explain(Plutinos, hot main belt)– non-adiabatic migration (Gomes, 2003)

• Inclination–size correlation– hot population formed closer to the Sun

• The edge at ∼ 50 AU– stellar encounter =⇒ p. 13– primordial edge at∼ 30 AU, KBOs pushe

out by the 2:1 (Levison & Morbidelli 2003

• The extended scattered disk– lost/rogue planets =⇒ p. 14– long term chaotic diffusion =⇒ p. 15– stellar encounter

• Mass loss ∼ 99%?!

11

Survival rate of Plutinos and Twotinos

from Tiscareno (PhD thesis, 2004)

12

Stellar encounter – perturbations on Kuiper Belt

from Ida, Larwood & Burkert (2000)

13

Origin of extended–SDOsRogue planets?

from Morbidelli & Levison (2004)14

Origin of extended–SDOsLong term chaos – ‘Arnold diffusion’?

from Malhotra (2004, in preparation)15

Dust from the Kuiper BeltPresent-day distribution

model from Moro-Martin & Malhotra (2003)

• Dust density measured to be nearly constantin outer solar system (Pioneer 10,11; Voyagers1,2)

• KB dust production rate (1µm < R < 1mm)' 1× 1015 g y−1 (Landgraf et al 2002)(eqv. D ≈ 1 km comet ground to dust everyyear)

• Small particles (R . 0.5µm) are blown out byradiation pressure

• Bound dust grains spiral inward underPoynting-Robertson (PR) drag– temporary trapping in Neptune’s MMRs

produces azimuthal structure

• Gravitational scattering by Jupiter and Saturnejects most particles– very small fraction of KB dust grains enter

the inner solar system(“inner hole” in the KB debris disk)

16

A History of Kuiper Belt Dust

• Theoretical models of Uranus-Neptuneformation suggest a total mass∼50M⊕ ina dynamically cold planetesimal disk, anda planet formation timescale∼107 yr (eg,Goldreich et al, 2004)– A collisional cascade in that disk would

produce dust at a rate 4–5 orders ofmagnitude larger than present

• The planets were mobilized towards theend of their formation, U-N undergoingoutward migration fuelled by the outerplanetesimal debris

• Shortly prior to the start of the migration,some mechanism disturbed the outerplanetesimal disk, exciting the e’s and i’s,perhaps stripping off the disk beyond ∼50AU– this event would have also caused a

‘spike’ in the dust production rate

• Thereafter, a rapid depletion ofplanetesimals led to a decline in the dustproduction rate

Planet accretion

Nep migration

A schematic history of the outer solar system dust productionrate

17


Recommended