Space Telescope Symposium May 2005 Planetary Dynamics: Chaos & Cleanup 1 Space Telescope Symposium May 2005 From observations of our own and other systems.

Slides:



Advertisements
Similar presentations
Resonant Structures due to Planets Mark Wyatt UK Astronomy Technology Centre Royal Observatory Edinburgh.
Advertisements

Star & Planet Formation Minicourse, U of T Astronomy Dept. Lecture 5 - Ed Thommes Accretion of Planets Bill Hartmann.
Asteroid Resonances [2] Kuliah AS8140 Fisika Benda Kecil Tata Surya dan AS3141 Benda Kecil dalam Tata Surya Budi Dermawan Prodi Astronomi 2006/2007.
Origins of Regular and Irregular Satellites ASTR5830 March 21, :30-1:45 pm.
Planetary Migration and Extrasolar Planets in the 2:1 Mean-Motion Resonance (short review) Renate Zechner im Rahmen des Astrodynamischen Seminars basierend.
Kozai Migration Yanqin Wu Mike Ramsahai. The distribution of orbital periods P(T) increases from 120 to 2000 days Incomplete for longer periods Clear.
Planet Formation Topic: Orbital dynamics and the restricted 3-body problem Lecture by: C.P. Dullemond.
Stability of Earthlike Planets in the Habitable Zones of five Extrasolar Systems Renate Zechner 6 th Alexander von Humboldt Colloquium for Celestial Mechanics.
Multi-planetary systems:.  Binaries  Single Star and Single Planetary Systems  Multi-planetary systems.
Secular, Kozai, mean-motion resonances D.N.C. Lin Department of Astronomy & Astrophysics University of California, Santa Cruz Lecture 4, AY 222 Apr 11th,
Planet Formation Topic: Resonances Lecture by: C.P. Dullemond Literature: Murray & Dermott „Solar System Dynamics“
Asteroid Resonances [1]
Planet Formation Topic: Formation of rocky planets from planetesimals Lecture by: C.P. Dullemond.
Status of RV Sub-Catelogy Norio Narita (NAOJ) Yasuhiro H. Takahashi (Univ. of Tokyo) Bun’ei Sato (Titech) Ryuji Suzuki (NAOJ) and SEEDS/HiCIAO/AO188 teams.
Dynamics of the young Solar system Kleomenis Tsiganis Dept. of Physics - A.U.Th. Collaborators: Alessandro Morbidelli (OCA) Hal Levison (SwRI) Rodney Gomes.
Chaos-assisted capture in the formation of Kuiper-belt binaries Sergey Astakhov UniqueICs, Saratov, Russia and NIC Forschungszentrum Jülich,Germany Ernestine.
1 Why exoplanets have so high eccentricities - By Line Drube - November 2004.
The `Nice’ Model Öpik approximation Planet migration in a planetesimal disk The Nice model Consequences of the Nice Model: Epoch of Late Heavy Bombardment,
Some 3 body problems Kozai resonance 2 planets in mean motion resonance Lee, M. H
On the determination of the probability of collisons of NEAS with the planets MACE 2006 Rudolf Dvorak ADG, Institute of Astronomy University of Vienna.
Fabio Antonini Joshua Faber Alessia Gualandris and David Merritt Rochester Institute of Technology.
Ge/Ay133 Planetary Dynamics. Orbital elements (3-D), & time evolution:
Reflected Light From Extra Solar Planets Modeling light curves of planets with highly elliptical orbits Daniel Bayliss, Summer Student, RSAA, ANU Ulyana.
Ge/Ay133 How do planetesimals grow to form ~terrestrial mass cores?
Numerical Simulations of the Orbits for Planetary Systems: from the Two-body Problem to Orbital Resonances in Three-body NTHU Wang Supervisor Tanigawa,
Based on the definition given by Kasting et al. (1993). The Habitable Zone.
Study the dynamics of KBOs --- using restricted three-body model Yeh, Lun-Wen
COMETS, KUIPER BELT AND SOLAR SYSTEM DYNAMICS Silvia Protopapa & Elias Roussos Lectures on “Origins of Solar Systems” February 13-15, 2006 Part I: Solar.
The Transit Method When a planet crosses in front of its star as viewed by an observer, the event is called a transit. Transits produce a very small change.
Gravity & orbits. Isaac Newton ( ) developed a mathematical model of Gravity which predicted the elliptical orbits proposed by Kepler Semi-major.
The long-term evolution of planetary orbits TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAAAAAA.
Astronomy: The Original Science STUDYING SPACE. Modern Calendar Based on observations of bodies in our solar system.
Chaotic Case Studies: Sensitive dependence on initial conditions in star/planet formation Fred C. Adams Physics Department University of Michigan With:
Stability of Extra-solar Planetary Systems C. Beaugé (UNC) S. Ferraz-Mello (USP) T. A. Michtchenko (USP) USP-UNC team on Exoplanets:
History of Astronomy - Part II
Planets in Debris Disks Renu Malhotra University of Arizona Planet-Debris co-evolution Where can debris exist? Cases: Solar system, upsilon Andromedae,
1B11 Foundations of Astronomy Extrasolar Planets Liz Puchnarewicz
Introductory Astronomy History – Solar Nebula 1. Dust to Planetesimals Grains of dust (solids) collide and adhere Larger grains grow to 10 9 planetesimals.
Modeling Planetary Systems Around Sun-like Stars Paper: Formation and Evolution of Planetary Systems: Cold Outer Disks Associated with Sun-like Stars,
Explorations of the Outer Solar System B. Scott Gaudi Harvard-Smithsonian Center for Astrophysics.
Dynamics of Extra-solar Planetary Systems with Hot Jupiters C. Beaugé (UNC) S. Ferraz-Mello (USP) T. A. Michtchenko (USP) USP-UNC team on Exoplanets:
Institute for Astronomy University of Vienna Stable planetary orbits in multiple planetary systems.
Alice Quillen University of Rochester Department of Physics and Astronomy Oct, 2005 Submillimet er imaging by Greaves and collaborato rs.
Gravity and Orbits   Newton’s Law of Gravitation   The attractive force of gravity between two particles   G = 6.67 x Nm 2 /kg 2 Why is this.
ASEN 5050 SPACEFLIGHT DYNAMICS Two-Body Motion Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 3: The Two Body Problem 1.
Extra Solar Planet Detection by the Doppler Detection method The following slides are a summary of the classroom presentation annotating the Doppler Detection.
Resonances. Resonances I. Orbital Resonances A. Definition: An orbital resonance occurs when two orbiting bodies exert a _______ and ________ gravitational.
Kepler’s Laws of planetary motion Newton’s law of universal gravitation Free fall acceleration on surface of a planet Satellite motion Lecture 13: Universal.
Occultation Studies of the Outer Solar System B. Scott Gaudi (Harvard-Smithsonian Center for Astrophysics)
Chaotic Dynamics of Stellar Spin in Binaries and the Production of Misaligned Hot Jupiters Natalia Storch, Kassandra Anderson & Dong Lai Cornell University.
DYNAMICAL EVOLUTION OF THE SEINAJOKI ASTEROID FAMILY Vladimir Đošović Bojan Novaković The sixth Symposium "Mathematics and Applications" 17. October2015.
Planets around Stars Beyond the Main Sequence (Evolved Stars) 1.RV measurements of Giant Stars 2.Timing Variations a)Pulsar Planets b)Planets around oscillating.
Copyright © 2010 Pearson Education, Inc. Clicker Questions Chapter 13 Neutron Stars and Black Holes.
Astronomy: A Beginner’s Guide to the Universe Seventh Edition © 2013 Pearson Education, Inc. Neutron Stars and Black Holes Chapter 13 Clickers.
Companion Candidates around Transiting Planetary Systems: SEEDS First/Second Year Results Norio Narita (NAOJ) Yasuhiro H. Takahashi (Univ. of Tokyo) and.
Collision Enhancement due to Planetesimal Binary Formation Planetesimal Binary Formation Junko Kominami Jun Makino (Earth-Life-Science Institute, Tokyo.
Celestial Mechanics VI The N-body Problem: Equations of motion and general integrals The Virial Theorem Planetary motion: The perturbing function Numerical.
Timing Transits to Find Extrasolar Earths Eric Agol, Jason Steffen (UW) Re’em Sari (Caltech) Will Clarkson (Southampton) (MNRAS, in press)
Celestial Mechanics VII
Resonances I. Orbital Resonances A. Definition: An orbital resonance occurs when two orbiting bodies exert a _______ and ________ gravitational influence.
Figure 4. Same as Fig. 3 but for x = 5.5.
Capture of Irregular Satellites during Planetary Encounters
Planetary system dynamics
Masaya M. Saito Institute of Statistical Mathematics
Signatures of formation mechanisms in the multiple-star statistics
A Solar System is Born.
Binary Stars Palomar Observatory.
The Structure of the Solar System
Planetary Dynamics Ge/Ay133.
Presentation transcript:

Space Telescope Symposium May 2005 Planetary Dynamics: Chaos & Cleanup 1 Space Telescope Symposium May 2005 From observations of our own and other systems we know: Secular resonances occur Mean motion resonances occur Chaotic motion occurs Collisions occur We suspect Ejections occur

Space Telescope Symposium May 2005 Planetary Dynamics: Chaos & Cleanup POrbital Period asemimajor axis nMean motion Mean longitude (=nt) Longitude of periapse Mass ratio m p /m * r H Hill radius = (/3) 1/3 a 1 Space Telescope Symposium May 2005

Planetary Dynamics: Chaos & Cleanup 1.Secular resonance: p-q’= const. 2. Kozai resonance: d/dt = 0 3. Close Encounters (r ~ Hill radius) 4. Two body mean motion resonances: pq’=const. 5. Three body mm resonances: pq’-r’’=const. 1 Space Telescope Symposium May 2005

Secular Instability Time Scales 1. Secular: T sec ~ P/ 2. Kozai: T koz ~ P (m 0 /m 2 )(a 2 /a) 3 where m 2 and a 2 are the mass and semimajor axis of the binary companion 3

Space Telescope Symposium May 2005 A Secular Resonance 4

Space Telescope Symposium May 2005 Consequences of the Kozai Instability 1. Large eccentricity, some of the time 2. Massive planets at small a 5

Space Telescope Symposium May 2005 HD 80606: Kozai? 6 Wu & Murray ApJ, 589, 605 (2003)

Space Telescope Symposium May 2005 Short Period Massive Planets 7 Wu & Murray ApJ, 589, 605 (2003)

Space Telescope Symposium May 2005 Crossing and Mean Motion Time Scales 1. Orbit crossing: T ej ~ P/(4 5/3 ) ~ 3x10 5 (P/12) (M J /M) 5/3 yrs 2. Mean Motion: T mm ~ P/(16e 2q ) e is initial free eccentricity, q=1,2,… For q>1, T mm >T ej 8

Space Telescope Symposium May 2005 Mean Motion Resonances 9

Space Telescope Symposium May 2005 Three Body Mean Motion Time Scales T tb ~ P/(    e 2q ) e is a representative initial free eccentricity, q=1,2,… For the outer solar system T tb ~ 10 8 yrs 10

Space Telescope Symposium May 2005 Three-body Resonances Holman & Wisdom AJ, 105, 1987 (1993)

Space Telescope Symposium May 2005 Consequences of Instability 1.Ejection/accretion, usually of lighter body 2. Remnant has substantial eccentricity 3. Larger separation between survivors, so the system tends to be more stable. Note however that there are other ways to produce dynamically stable spacings and substantial eccentricities 12

Space Telescope Symposium May 2005 Consequences of Instability? 13