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Rosemary Mardling

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Title: Rosemary Mardling


1
School of Mathematical Sciences
Rosemary Mardling
2
Planetary Dynamics
  • Planet formation
  • assembling terrestrial planets and giant cores
  • Close encounters and collisions between
    planetesimals (unstable orbits)
  • Gravitational influence of existing giant planets
  • planet-disk interaction (tidal interaction) (hot
    Jupiters - migration)
  • secular and dynamical stability (resonance)
  • resonance capture (eg. 21 extrasolar planets)
  • moon formation (in situ and capture/collision)
    (web animation-Kokubo)
  • effect of binary companion

3
Planetary Dynamics
  • Small bodies in the Solar System
  • asteroid belt
  • resonant structure (Kirkwood gaps)
  • stability

4
Planetary Dynamics
  • Small bodies in the Solar System
  • Kuiper belt (old and scattered)
  • resonant structure (32v 21?)
  • stability
  • edge
  • Comets (high e, unstable)
  • Dust (debris disks)

5
Planetary Dynamics
  • Long-term stability
  • Is the Solar System stable?
  • Secular resonance
  • resonance and chaos

6
Planetary Dynamics
  • non-point mass dynamics
  • Tidal and spin-orbit coupling
  • Planet-moon interactions
  • Star-planet interactions (hot Jupiter companion
    planet)
  • Planet-disk interactions
  • Planet-ring-moon interactions (Saturns rings and
    shepherds)
  • Star-planet-moon (Sun-Earth-Moon)

7
Planetary Dynamics
  • other phenomena
  • relativistic potential of star (post-Newtonian)
  • Apsidal advance of Mercury
  • Survival of short-period terrestrial planets
  • Kozai cycles
  • Large oscillations in eccentricity (up to unity)
  • and inclination caused by inclined binary
    companion

8
  • NUMERICAL METHODS
  • symplectic integration (energy conserved)
  • Hermite with regularization for close encounters
    (N-body)
  • hydrodynamical codes
  • rubble piles of sticky particles (N-body)
  • direct integration with additional accelerations
    (tides, spin, GR)
  • orbit-averaging with additional accelerations
  • Lyapunov exponents (chaosinstability)

9
  • ANALYTICAL METHODS
  • Circular restricted planar three-body problem
  • One body massless
  • Other body small compared to primary
  • Perturbation methods
  • Small eccentricities and inclinations
  • Small masses compared to primary
  • New formalism which drops these restrictions

10
  • Extrasolar planets many hot Jupiters
  • many planets with high eccentricities
  • 9 systems with two or more planets
  • 2 with three planets
  • 2 systems in 21
    resonance
  • 1 system in 31 resonance
  • Planet formation questions
  • What kind of planetary systems is the star
    formation process
  • capable of producing?
  • What can observed systems tell us about the
    planet formation process?
  • What kind of structures can we expect from
    disk-like systems
  • prograde motion, small inclinations
  • Lots of opportunity for resonance

11
  • Planet formation questions
  • Do non-coplanar systems exist?
  • how does the cluster environment affect
    configuration?
  • How common are systems like the Solar System?
  • small eccentricites, inclinations
  • Terrestrials inner, giants outer
  • not much migration
  • Is the edge of the Solar System due to a
    passing star?
  • Are we certain planets cannot form close to star?
  • migration
  • scattering

12
Question
Why is resonance associated with stability AND
instability???
  • Asteroid belt gaps associated with resonances
  • Kuiper belt bodies safe in resonances with
    Neptune
  • (example Pluto)

A resonance can be a safe harbour or a stormy
sea. WHY?
13
Linear resonance (damped)
response curve
Resonance width DEFINED as full width half max
14
The three-body problem
Easy to write down but hard to extract secrets!
Lots of symmetry to take advantage of
15
Jacobi coordinates (hierarchies)
--- responsible for all interesting behaviour!
16
Spherical harmonic expansion to identify
resonance angles
In practice we keep l2,3 quadrupole and
octopole terms
17
Fourier analysis
18
Identify resonance angle
resonance angle
Away from resonance, short-period terms
time-average to zero. nn0 terms responsible
for secular evolution.
19
Secular evolution Upsilon Andromedae
no energy exchanged
semi-major axes
eccentricities
20
short-period variations
orbital variation of inner planet over 3 years
21
resonance
2 planets 21 resonance Tout 2 Tin
Energy exchange tends to be in same direction at
conjunction
THEY ARE CAPABLE OF EXCHANGING ENERGY
22
resonance
non-resonant system
resonant system
libration
circulation
23
resonance
resonance width has precise meaning
24
resonance
Resonance width twice separatrix amplitude
25
resonance overlap
KAM, Chirikov
chaos
dots translate to stability boundary
n1 resonances
26
n1 resonances
27
Smaller masses skinnier resonances
But n2 resonances important for extreme mass
ratios these are missing from this plot
28
Thus a resonance can be a safe haven if there are
no other resonances overlapping
There are many resonant orbits in the Solar
System many were formed when the protoplanetary
disk was present -- dissipation nonlinear
fixed points RESONANCE CAPTURE
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