Impact of Self-Gravity at the Encke Gap Edge Abstract We present the results of several numerical simulations of the outer edge of the Encke gap that include.

Slides:



Advertisements
Similar presentations
Saturn The Ringed Planet Very nice title slide. Ive got a few suggestions to make it better though. Your title can be simplified. Also, the contrast between.
Advertisements

Planetary Rings All four jovian planets have ring systems girdling their equators. Many of the inner jovian moons orbit close to (or even within) the parent.
Unt4: asteroid part 2. Comets Comet Ikeya-Seki in the dawn sky in 1965.
The Radial Variation of Interplanetary Shocks C.T. Russell, H.R. Lai, L.K. Jian, J.G. Luhmann, A. Wennmacher STEREO SWG Lake Winnepesaukee New Hampshire.
Chemical Models of Protoplanetary Disks for Extrasolar Planetary Systems J. C. Bond and D. S. Lauretta, Lunar and Planetary Laboratory, University of Arizona.
Calibration Scenarios for PICASSO-CENA J. A. REAGAN, X. WANG, H. FANG University of Arizona, ECE Dept., Bldg. 104, Tucson, AZ MARY T. OSBORN SAIC,
Physical processes within Earth’s interior Topics 1.Seismology and Earth structure 2.Plate kinematics and geodesy 3.Gravity 4.Heat flow 5.Geomagnetism.
Lecture 4 Physics in the solar system. Tides Tides are due to differential gravitational forces on a body.  Consider the Earth and Moon: the gravitational.
Planetary Ring Systems. Rings: A B C 4/4 Giant Worlds Have Rings Jupiter: broad, dark, fine particles Saturn: broad, bright, complex, icy particles.
10Nov2006 Ge/Ay133 More on Jupiter, Neptune, the Kuiper belt, and the early solar system.
NJIT Physics 320: Astronomy and Astrophysics – Lecture XIII Carsten Denker Physics Department Center for Solar–Terrestrial Research.
Wavelike Structure in Saturn’s Rings
PTYS/ASTR 206Rings / Galilean Satellites 4/10/07 Planetary Rings (cont.) + Galilean Satellites.
Ge/Ay133 How do planetesimals grow to form ~terrestrial mass cores?
The most distant planet known to the ancients is NASA’s latest target for exploration.
Saltation Impact as a Means for Raising Dust on Mars By Ronald Greeley.
Lecture 34 The Outer Planets. The Moon. The Origin of the Moon The Outer Planet Family Chapter 16.9 
© 2011 Pearson Education, Inc. Chapter 6 The Solar System.
9.2 Comets Our Goals for Learning How do comets get their tails? Where do comets come from?
Survey of the Solar System
Copyright © 2010 Pearson Education, Inc. The Jovian Planets Jupiter, Saturn, Uranus, Neptune.
The Forces that Sculpt Saturn’s Rings…. Matt Hedman Cassini ISS team Cassini VIMS team CHARM telecon
This is the ATTRACTIVE force exerted between objects
Our Solar system YouTube - The Known Universe by AMNH.
© 2011 Pearson Education, Inc. Chapter 6 The Solar System.
SHINE SEP Campaign Events: Long-term development of solar corona in build-up to the SEP events of 21 April 2002 and 24 August 2002 A. J. Coyner, D. Alexander,
Nova. Nova – Rapid increase in luminosity of a white dwarf in a binary system The Roche lobe is the region of space around a star in a binary system within.
Analysing Lunar Craters using data from the Liverpool Telescope.
High Mass Stellar Evolution Astrophysics Lesson 13.
20 NOVEMBER 2007 CLASS #23 Astronomy 340 Fall 2007.
Chapter 7 Rotational Motion and The Law of Gravity.
Outer Planets  Comparative Giant Planets  Jupiter  Saturn  Uranus  Neptune  Gravity  Tidal Forces Sept. 25, 2002.
1B11 Foundations of Astronomy The Jovian Planets Silvia Zane, Liz Puchnarewicz
Jupiter (Galileo) Saturn (Cassini) Uranus (Hubble) Neptune (Voyager)
Ring- Moon Interactions 16 November Shepherd Satellites of F ring.
All Late Work Due by 12/18/15.
Moon and Rings 13. Astronomy Picture of the Day Moons of Jovian Planets Jupiter alone has over 60 We will focus on large: Diameter > 2,500 km Why study.
Chapter 11 The Interstellar Medium
 Understand how our view of the solar system has changed over time and how discoveries made have led to our changing our view of the solar system. 
Copyright © 2010 Pearson Education, Inc. Chapter 16 Galaxies and Dark Matter Lecture Outline.
Comparative Planetology
Today’s APODAPOD  Chapter 9 – Outer Planets  Quiz 8 this week ONLINE Friday  Kirkwood TONIGHT??, 7-9PM  Homework due FRIDAY The Sun Today A100 Saturn.
Chapter 13 Uranus and Neptune. Uranus was discovered in 1781 by Herschel; first planet to be discovered in more than 2000 years Little detail can be seen.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 7 The Jovian Planets.
Review Worksheet Solutions. 1. Describe the focus of comparative planetology and discuss its importance to solar system studies. Comparative planetology.
Boom and Bust Cycles in Saturn’s Rings? Larry W. Esposito LASP, University of Colorado 23 February 2010.
∆G.P.E = mg∆h When you have previously considered gravitational potential energy, you would have used the equation: Consider a monkey climbing 2 metres.
Section 4: Earth’s Moon. What are we learning about today? 1. What features are found on the moon’s surface? 2. What are some characteristics of the moon?
Gravity 3/31/2009 Version. Consent for Participation in Research Construct Centered Design Approach to Developing Undergraduate Curriculum in Nanoscience.
Micro-structural size properties of Saturn’s rings determined from ultraviolet measurements made by the Cassini Ultraviolet Imaging Spectrograph Todd Bradley.
Chapter 7 Rotational Motion and The Law of Gravity.
Earth’s Moon - using radar we find the distance to the Moon to be 384,000 km (this is the length of the orbit’s semi-major axis).
Cassini UVIS Observations and the History of Saturn’s Rings Larry W. Esposito, Joshua E. Colwell, Glen R. Stewart LASP, University of Colorado 24 August.
Meteors vs. Meteorites
© 2017 Pearson Education, Inc.
The Jovian Planets.
Motions of the Moon, Phases and Eclipses (Ch 3)
Review: the giant planets and their moons
Saturn and its ring.
Bonnie Meinke UVIS team meeting January 5, 2010
Cassini UVIS Observations: Structure and History of Saturn’s Rings
Astronomy 405 Solar System and ISM
Living at the Edge of Saturn’s Rings
Tides & Rings.
Understand the movement of planetary bodies.
Collisional formation of ringlets in high M resonances
Regolith Growth and Darkening of Saturn’s Ring Particles
Comparing F ring to B ring outer edge: implications for accretion
Althea V. Moorhead, University of Michigan
Please don’t touch the beads or string!!!
Presentation transcript:

Impact of Self-Gravity at the Encke Gap Edge Abstract We present the results of several numerical simulations of the outer edge of the Encke gap that include collisions and particle self-gravity. There are a number of significant interactions between the moon-induced wakes and the gravity wakes. In this poster we focus primarily on features that form at the edge of the ring, how those features might evolve over multiple synodic periods, and how these various features might appear in Cassini observations. The primary features seen in the edge region include a thickening of material that appears to fuel an increase in the strength of the gravity wakes. In our simulation, the gravity wakes are seen to grow as long as 3-km in length, more than 10 times longer than normal. These structures form as the particles move out into the gap after the moon wakes produce a high- density region. They are destroyed and re-form as the ring particles move along the wavy edge of the gap. Multiple Synodic Periods Recently we performed a simulation that ran for more than one synodic period. This simulation involved 125,000 particles each with a radius of 7.5 m and internal density of 0.5 g/cm 3 giving a surface density of 62.9 g/cm 2 and maintaining the same geometric optical depth of the other simulations. These figures show that simulation during the first and second synodic periods at similar distances after the moon encounter. Unfortunately, that choice of conditions resulted in a weaker edge effect that was not compounded with a second pass by the moon. We are currently extending simulation C beyond a synodic period to see if the effected region grows or strengthens in that situation. Different Systems These figures show the behavior of several different systems at different points in the simulation. All the simulations shared an optical depth of Next to each row of figures is the number of particles, internal particle density, and average surface density of the simulation. Measurements from Voyager images gives surface densities in the A ring between 26±10 and 96±40 g/cm 2 Annotated Simulation Cell This figure shows a detailed view of one frame of simulation C. The major features are labeled to help you understand what is happening in these simulations. Conclusions Gravity and moon wakes can potentially interact in complex ways in planetary rings. The the types of structures that we see in these simulations have been seen in some of the early Cassini images. The behavior of these features is strongly impacted by the nature of the particles in the ring so it is possible that it could be a useful diagnostic if observations can be compared to a sufficiently broad sampling of simulations. Icarus Paper – many of the results shown here appear in a paper recently accepted to Icarus. If you would like a preprint of that paper, please ask and we can provide you with one. Detailed Time Sequence These figures from the same simulation that was shown above illustrate how these structures form and evolve over an orbital period. Particle Count: Particle Radius: 10.64m Internal Density: 0.7g/cm 3 Surface Density: 124.6g/cm 2 Particle Count: Particle Radius: 10.64m Internal Density: 0.5g/cm 3 Surface Density: 89.0g/cm 2 Particle Count: Particle Radius: 5.32m Internal Density: 0.7g/cm 3 Surface Density: 62.3g/cm 2 Particle Count: Particle Radius: 5.32m Internal Density: 0.5g/cm 3 Surface Density: 44.5g/cm 2 Particle Count: Particle Radius: 2.66m Internal Density: 0.5g/cm 3 Surface Density: 22.3g/cm 2 Particle Count: Particle Radius: 5.32m Internal Density: 0.0g/cm 3 Surface Density: 0.0g/cm 2 Pan wakes propagating outward Clumps stringing off a wake after being tightly packed Oversized gravity wakes formed from synchronized motion in higher density region. Few gravity wakes between Pan wakes Mark C. Lewis (Trinity University) Glen R. Stewart (Laboratory for Atmospheric and Space Physics) Ratio of Radial Distance from Moon to Orbit Radius of Moon