celestial mechanics: from asteroids to extrasolar planets

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Celestial Mechanics: from Asteroids to Extrasolar Planets 23.06.2010 :: Florian Freistetter :: OATS

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Page 1: Celestial Mechanics: from Asteroids to Extrasolar Planets

Celestial Mechanics: from Asteroids to Extrasolar Planets

23.06.2010 :: Florian Freistetter :: OATS

Page 2: Celestial Mechanics: from Asteroids to Extrasolar Planets

Orbital Dynamics: Order and Chaos

since Poincaré (1889) we know that the n-body problem (n>2) can not be solved analytically and can give chaotic solutions

Part I: Chaotic Orbits of Near Earth Asteroids during the last 15 years ~450 extrasolar systems were

discovered – but it is still almost impossible to detect terrestrial planets

Part II: Stability of potential terrestrial planets in extrasolar systems

Part III: Planets and Asteroids in the disk of Beta Pictoris

Page 3: Celestial Mechanics: from Asteroids to Extrasolar Planets

Asteroids

0

5 0

1 0 0

1 5 0

2 0 0

1 2 3 4 5

num

be

r o

f ast

ero

ids

s e m i m a j o r a x i s [ A U ]

M e r c u r y V e n u s E a r t h M a r s J u p i t e r

3 : 1 8 : 3

5 : 2

1 : 1

3 : 2H i l d a s

T r o j a n s

2 : 1

4 : 1

H u n g a r i a s

A T E N s A M O R sA P O L L O s

N E A s

Page 4: Celestial Mechanics: from Asteroids to Extrasolar Planets

Chaotic Motion of NEAs

Close encounters -> Chaos!10563 Izdhubar

Page 5: Celestial Mechanics: from Asteroids to Extrasolar Planets

Chaotic Motion of NEAs

Longterm evolution of chaotic orbits

gives no meaningful results for single objects !

Page 6: Celestial Mechanics: from Asteroids to Extrasolar Planets

NEA Groups

2 important classifications: Shoemaker et al. (1973):

Aten :: Apollo :: Amor a, e (crossing behaviour)

Milani et al (1989) 7 classes Dynamical behaviour (encounters, etc)

How does Chaos effect the groups?

Page 7: Celestial Mechanics: from Asteroids to Extrasolar Planets

Mixing!

Chaos + Long Timescales = Problems!

Page 8: Celestial Mechanics: from Asteroids to Extrasolar Planets

Mixing

Object ↔ Group

Page 9: Celestial Mechanics: from Asteroids to Extrasolar Planets

Mixing

How much time does a NEA spend in its initial group?

• 69.86 % (Shoemaker et al. classification) (Dvorak & Freistetter 2001, Freistetter 2009)

• 65.72 % (Milani et al. classification) (Dvorak & Freistetter 2001, Freistetter 2009)

Need a new way of classification: Fuzzy Logic!

Page 10: Celestial Mechanics: from Asteroids to Extrasolar Planets

Fuzzy LogicAge: 32 years

•very young: 25%

• young: 50%

• not very young: 75%

• more or less old: 2%

• old: 0%

• very old: 0%

It is possible to be a member

of multiple groups with a

different degree!

Page 11: Celestial Mechanics: from Asteroids to Extrasolar Planets

Fuzzy Classification

Comparison with Milanis Classification

http://www.celestialmechanics.eu/neas/

Page 12: Celestial Mechanics: from Asteroids to Extrasolar Planets

Fuzzy Classification

• compare the classification data with the Spaceguard classes

Geographos group

• many close approaches with Earth

• some close approaches with Venus

• semimajor axis almost constant

(1620) Geographos:

• G1 (no mixing): 1

• G2 (Venus): 0.03

• G3 (Earth): 0.76

Oljato group

• chaotic orbits

• large eccentricities

• close encounters with all planets

(2201) Oljato:

• G1 (no mixing): 0.04

• G2 (Venus): 0.38

• G3 (Earth): 0.36

• G4 (Mars): 0.28

Fuzzy Classification works!

Page 13: Celestial Mechanics: from Asteroids to Extrasolar Planets

Extrasolar Planets

Observation of terrestrial planets? -> Theoretic simulations Stability in the habitable Zone

Page 14: Celestial Mechanics: from Asteroids to Extrasolar Planets

HD 41004 A

Star 1Mstar1 = 0.7 MSun

Planetm sin i = 2.3 Mjup

a = 1.31 AUe = 0.39 + 0.17ω ≈ 114o

Star 2m = 0.4 MSun

a = 21 AUe = 0.1

Page 15: Celestial Mechanics: from Asteroids to Extrasolar Planets

Influence of the companion

ebin=0.1 epl=0.22 no secondary epl=0.22

4:1 7:2 3:18:3

Page 16: Celestial Mechanics: from Asteroids to Extrasolar Planets

Different Methods

epl=0.22MEM FLI

Page 17: Celestial Mechanics: from Asteroids to Extrasolar Planets

Importance of observationsepl=0.24 epl=0.26 epl=0.28 epl=0.30

epl=0.32 epl=0.34 epl=0.36 epl=0.38

Page 18: Celestial Mechanics: from Asteroids to Extrasolar Planets

b Pictoris

spectral type: A5 V star age: ~20 Myrs mass: 1.75 MSUN

1984: debris disk!

Smith & Terrile 1984

first debris disk some 100 articles

Page 19: Celestial Mechanics: from Asteroids to Extrasolar Planets

The disk of b Pictoris

many interesting structures:

warp: → inclined planet? Mouillet et al.:

Page 20: Celestial Mechanics: from Asteroids to Extrasolar Planets

The disk of b Pictoris “Falling Evaporating Bodies (FEBs)”: variations in spectral lines → small bodies fall onto the star → planet has to disturb these bodies

Beust et al. 1990

Page 21: Celestial Mechanics: from Asteroids to Extrasolar Planets

The disk of b Pictoris clumps in the disk

Telesco et al. (2005) Okamoto et al. (2004)

Page 22: Celestial Mechanics: from Asteroids to Extrasolar Planets

Belt structures in the b Pic-disk A: ~6.4 AU [2] B: ~16 AU [1,2,4] C: ~32 AU [1,2,4] D: ~52 AU [1,3,4] structures in the outer disk

[1] Wahhaj et al 2003 [2] Okamoto et al. 2004[3] Telesco et al. 2005 [4] Golimowski et al. 2006

Can these clumps be caused by planetesimal belts? What planets are needed to con- fine such belts?

Page 23: Celestial Mechanics: from Asteroids to Extrasolar Planets

Planetesimal belts objects from 0.15 m – 7 km M

tot = 0.3MEARTH

a = 6 - 7 AU e = 0 - 0.1 → evolution of dust particles → Brightness

→ observed peaks can be due to planetesimal belts!

Page 24: Celestial Mechanics: from Asteroids to Extrasolar Planets

Planets

belts are confined by planets What are the parameter of the planet(s) so

that the perturbations cause the observed clumps?

simulations with 1 – 3 planets parameters (M, a, e, i) very varied

Page 25: Celestial Mechanics: from Asteroids to Extrasolar Planets

One Planet

Page 26: Celestial Mechanics: from Asteroids to Extrasolar Planets

Two Planets

Page 27: Celestial Mechanics: from Asteroids to Extrasolar Planets

Three Planets

Page 28: Celestial Mechanics: from Asteroids to Extrasolar Planets

Summary Confirmation of

previous results Additional

restrictions for planetary parameters

At least 3 planets are needed to explain observations

The planetary system could be resonant

Page 29: Celestial Mechanics: from Asteroids to Extrasolar Planets

Beta Pictoris b Do the planets

exist?

Page 30: Celestial Mechanics: from Asteroids to Extrasolar Planets

Beta Pictoris b

Page 31: Celestial Mechanics: from Asteroids to Extrasolar Planets

E N D