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Planetary Dynamics Ge/Ay133.

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Presentation on theme: "Planetary Dynamics Ge/Ay133."— Presentation transcript:

1 Planetary Dynamics Ge/Ay133

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3 Orbital elements (3-D), & time evolution:

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24 What ARE Lyapounov exponents and times?
Suppose that two orbits are separated in phase space by d, and that d follows d = d0 e-g(t-t0) G is the Lyapounov exponent, and 1/g is the Lyapounov time. Numerically, G = lim ln(d/d0)/(t-t0) As t → ∞. For regular orbits, g → 0. Regular ↑ Chaotic ↓

25 Libration Rotation Chaos in the outer S.S.: Uranus’s orbit can go from librating to rotating behavior. Chaotic, but

26 The exact details are sensitive to the presence or
absence of remnant gas or planetesimal disks: As disks dissipate, a stable system can become unstable…

27 Recall: Resonant systems common, & migrate more slowly in a disk…
From Armitage. Why? Couple of reasons, including wider gap opening and exchange of momentum between the interacting planets & disk.

28 Might this explain some of the unusual exo-planets?
Simulation of two-planet interactions, with slow outer planet migration: HD 12661

29 Are HD 12661 and/or Ups And “apsidally locked”?

30 More recent analyses suggest eUpsAndc is variable!

31 Need an impulsive scatterer. As disk disperses,
lose planet?


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