Angular Momentum in the Kuiper Belt

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Angular Momentum in the Angular Momentum in the Kuiper Belt Kuiper Belt Scott S. Sheppard Carnegie Institution of Washingt Department of Terrestrial Magnet

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Angular Momentum in the Kuiper Belt. Scott S. Sheppard Carnegie Institution of Washington Department of Terrestrial Magnetism. Main Asteroid Belt 24 > 200 km. Trojan Asteroids 2 ~ 200 km. Kuiper Belt 10,000 > 200 km. Size Comparison of Rocky/Icy Bodies in the Solar System. - PowerPoint PPT Presentation

Transcript of Angular Momentum in the Kuiper Belt

Page 1: Angular Momentum in the  Kuiper Belt

Angular Momentum in the Angular Momentum in the Kuiper BeltKuiper Belt

Scott S. Sheppard

Carnegie Institution of WashingtonDepartment of Terrestrial Magnetism

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Main Asteroid Belt24 > 200 km

Trojan Asteroids2 ~ 200 km

Kuiper Belt10,000 > 200 km

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Gravitational Self Compression > Material Strength

Primordial Distribution of Angular Momentum

For Diameters > 200 km:

- Early Collisional environment

Size Comparison of Rocky/Icy Bodies in the Solar System

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Dynamical Classes in the Outer Solar System

Dynamically Disturbed and Collisionally Processed.

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Sedna

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Plan View of the Kuiper Belt

Brightest KBO is19th magnitude

Diameter > 200 kmMag < 22.5

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Overview of DataSample of over 40 large KBOs

1) Light curves

2) Phase curves

UH 2.2m

-> Shapes-> Surface Characteristics-> Densities-> Binaries-> Angular Momenta-> Outgassing

du Pont 2.5m

Short and Long Term Variations

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Short-term Variability

2000 GN171

1. Albedo2. Elongation3. Binary

2000 GN171 period = 7.9 hours

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29% > 0.15 mags18% > 0.40 mags12% > 0.60 mags

KBOs (40 in sample)

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1. Albedo effects are usually only 10 to 20% (Degewij et al. 1979)

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2. Elongation

Rotational Triaxial Ellipsoids (Jacobi Ellipsoids)

Fast Rotations < 7 hours

For large objects (> 200 km)

Spherical Gravitational Compression > Material Strength

Triaxial elongation from rotational angular momentum

(Leone et al. 1984)

P = (3 Pi / G rho)1/2

crit

Centripetal acceleration = gravitational acceleration

As angular momentum increases an object will go frombeing a sphere to biaxial to

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a/b = 100.4 x delta mag

Axis Ratio from rotationallight curve:

Period and amplitude can be related to an objects density

Varuna

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Jewitt and Sheppard 2002

Varuna Density ~ 1100 kg/m 3

Assume Rotationally distortedStrengthless Rubble Pile

Cosmochemically PlausibleRock Fraction ~ 0.5

Porosity ~ 10 to 20%

Chandrasekhar 1987Leone et al. 1984

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1999 TC36

3. Eclipsing Binaries

-Probability of eclipse events to our line of sight decreases as the separation increases

-Tidal interactions distort close components

Photometric Range Max ~ 0.75 mags

Photometric Range Max ~ 1.2 mags(Leone et al. 1984)

(Trujillo and Brown 2002)

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2001 QG298 Period = 13.7744 hoursRange = 1.1 mags

Diameter ~ 250 km

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2001 QG298 HektorKleopatra

2001 QG298 is only the 3rd known minor planet with diameter > 50 km and a photometric range > 1 magnitude

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Trojan Asteroid 624 Hektor

Main Belt Asteroid 216 Kleopatra

KBO 2001 QG298

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Merline, Dumas and Menard 1999

CFHT Adaptive Optics images of Kleopatra

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Sheppard and Jewitt 2004

Comparison of Large Main Belt Asteroids and Kuiper Belt Objects

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Margot 2002

Comparison of typical binary systems within the Solar System.

100 km

100 km

1 km

20,000 km

1000 km

2.5 km

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Funato et al. 2004

KBO Binary Formation Mechanisms:

TidalDisruption

DirectCollisions

Three BodyInteractions

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Known Binaries of Large Minor Planets in the Solar System

Does a largeangular momentumof the primarycorrespond tosatellite formation?

Current angularMomentum ofLarge objects hintsAt an earlier denserKuiper Belt.

Maybe 100 times more dense.

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Noll et al. (2002) found about 4% of KBOs were binary with separations > 0.15”

We find 5 of 34 KBOs are in the close, similar component, eclipsing binary region (15%)

Consistent with Goldreich et al. (2002) model of binary formation but not with the Weidenschilling model (2002)

Collisionless interactionsIn a denser Kuiper BeltDuring the formation epoch.

- Dynamical Friction would create more close in binaries

(Because of projection effects, the fraction may be much larger)

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Conclusions- Many Kuiper Belt Objects have large amplitude light curves

- Some may be rotationally deformed rubble piles- Many are probably contact or nearly contact binaries

- Kuiper Belt must have been about 100 times more dense in the distant past to explain current amount of angular momentum we see.

- Binary formation is still unclear, but direct collisions may have be an important factor.

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Short and Long Term Variability

Consecutive Nights

Multiple Months

Absolute Photometry

Mag = Msun – 2.5 log(albedo x radius x phase / heliocentric x geocentric )2 2 2

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Period = 8.08 hours

Period = 4.04 hours

1995 SM55

V-R=0.38

Single-peak

Double-peak

Binary or Cometary orComplex Rotation?

t = u Q / p K r w

Damping time scale

2 3

u is rigidityQ is ratio energy in oscillation to that lost p is the densityK is irregularity of bodyr is the radiusw is angular frequency

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1. Nonuniform Surface Markings

Iapetus

Photometric Range ~ 0.3 mags

Photometric Range ~ 2 mags

B – V ~ 0.1 mags (Millis 1977)

-synchronous rotation

-atmosphere

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20000 Varuna Rotational Lightcurve (diameter ~ 900 km)

Period = 6.3442 hours

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20000 Varuna: Found No Color Variation with Rotation

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Asteroid and KBO Limiting Densities

Sheppard and Jewitt 2002

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5 KBOs can not be easily explained from albedo or rotational elongation