A Wunda-Full World? Carbon Dioxide Ice Deposits on Umbriel and Other Uranian Moons
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Cassini Update
Cassini Update Dr. Linda Spilker Cassini Project Scientist Outer Planets Assessment Group 22 February 2017 Sols%ce Mission Inclina%on Profile equator Saturn wrt Inclination 22 February 2017 LJS-3 Year 3 Key Flybys Since Aug. 2016 OPAG T124 – Titan flyby (1584 km) • November 13, 2016 • LAST Radio Science flyby • One of only two (cf. T106) ideal bistatic observations capturing Titan’s Northern Seas • First and only bistatic observation of Punga Mare • Western Kraken Mare not explored by RSS before T125 – Titan flyby (3158 km) • November 29, 2016 • LAST Optical Remote Sensing targeted flyby • VIMS high-resolution map of the North Pole looking for variations at and around the seas and lakes. • CIRS last opportunity for vertical profile determination of gases (e.g. water, aerosols) • UVIS limb viewing opportunity at the highest spatial resolution available outside of occultations 22 February 2017 4 Interior of Hexagon Turning “Less Blue” • Bluish to golden haze results from increased production of photochemical hazes as north pole approaches summer solstice. • Hexagon acts as a barrier that prevents haze particles outside hexagon from migrating inward. • 5 Refracting Atmosphere Saturn's• 22unlit February rings appear 2017 to bend as they pass behind the planet’s darkened limb due• 6 to refraction by Saturn's upper atmosphere. (Resolution 5 km/pixel) Dione Harbors A Subsurface Ocean Researchers at the Royal Observatory of Belgium reanalyzed Cassini RSS gravity data• 7 of Dione and predict a crust 100 km thick with a global ocean 10’s of km deep. Titan’s Summer Clouds Pose a Mystery Why would clouds on Titan be visible in VIMS images, but not in ISS images? ISS ISS VIMS High, thin cirrus clouds that are optically thicker than Titan’s atmospheric haze at longer VIMS wavelengths,• 22 February but optically 2017 thinner than the haze at shorter ISS wavelengths, could be• 8 detected by VIMS while simultaneously lost in the haze to ISS. -
Exomoon Habitability Constrained by Illumination and Tidal Heating
submitted to Astrobiology: April 6, 2012 accepted by Astrobiology: September 8, 2012 published in Astrobiology: January 24, 2013 this updated draft: October 30, 2013 doi:10.1089/ast.2012.0859 Exomoon habitability constrained by illumination and tidal heating René HellerI , Rory BarnesII,III I Leibniz-Institute for Astrophysics Potsdam (AIP), An der Sternwarte 16, 14482 Potsdam, Germany, [email protected] II Astronomy Department, University of Washington, Box 951580, Seattle, WA 98195, [email protected] III NASA Astrobiology Institute – Virtual Planetary Laboratory Lead Team, USA Abstract The detection of moons orbiting extrasolar planets (“exomoons”) has now become feasible. Once they are discovered in the circumstellar habitable zone, questions about their habitability will emerge. Exomoons are likely to be tidally locked to their planet and hence experience days much shorter than their orbital period around the star and have seasons, all of which works in favor of habitability. These satellites can receive more illumination per area than their host planets, as the planet reflects stellar light and emits thermal photons. On the contrary, eclipses can significantly alter local climates on exomoons by reducing stellar illumination. In addition to radiative heating, tidal heating can be very large on exomoons, possibly even large enough for sterilization. We identify combinations of physical and orbital parameters for which radiative and tidal heating are strong enough to trigger a runaway greenhouse. By analogy with the circumstellar habitable zone, these constraints define a circumplanetary “habitable edge”. We apply our model to hypothetical moons around the recently discovered exoplanet Kepler-22b and the giant planet candidate KOI211.01 and describe, for the first time, the orbits of habitable exomoons. -
Planetary Nomenclature: an Overview and Update
3rd Planetary Data Workshop 2017 (LPI Contrib. No. 1986) 7119.pdf PLANETARY NOMENCLATURE: AN OVERVIEW AND UPDATE. T. Gaither1, R. K. Hayward1, J. Blue1, L. Gaddis1, R. Schulz2, K. Aksnes3, G. Burba4, G. Consolmagno5, R. M. C. Lopes6, P. Masson7, W. Sheehan8, B.A. Smith9, G. Williams10, C. Wood11, 1USGS Astrogeology Science Center, Flagstaff, Ar- izona ([email protected]); 2ESA Scientific Support Office, Noordwijk, The Netherlands; 3Institute for Theoretical Astrophysics, Oslo, Norway; 4Vernadsky Institute, Moscow, Russia; 5Specola Vaticana, Vati- can City State; 6Jet Propulsion Laboratory, California Institute of Technology, Pasadena, California; 7Uni- versite de Paris-Sud, Orsay, France; 8Lowell Observatory, Flagstaff, Arizona; 9Santa Fe, New Mexico; 10Minor Planet Center, Cambridge, Massachusetts; 11Planetary Science Institute, Tucson, Arizona. Introduction: The task of naming planetary Asteroids surface features, rings, and natural satellites is Ceres 113 managed by the International Astronomical Un- Dactyl 2 ion’s (IAU) Working Group for Planetary System Eros 41 Nomenclature (WGPSN). The members of the Gaspra 34 WGPSN and its task groups have worked since the Ida 25 early 1970s to provide a clear, unambiguous sys- Itokawa 17 tem of planetary nomenclature that represents cul- Lutetia 37 tures and countries from all regions of Earth. Mathilde 23 WGPSN members include Rita Schulz (chair) and Steins 24 9 other members representing countries around the Vesta 106 globe (see author list). In 2013, Blue et al. [1] pre- Jupiter sented an overview of planetary nomenclature, and Amalthea 4 in 2016 Hayward et al. [2] provided an update to Thebe 1 this overview. Given the extensive planetary ex- Io 224 ploration and research that has taken place since Europa 111 2013, it is time to update the community on the sta- Ganymede 195 tus of planetary nomenclature, the purpose and Callisto 153 rules, the process for submitting name requests, and the IAU approval process. -
The Subsurface Habitability of Small, Icy Exomoons J
A&A 636, A50 (2020) Astronomy https://doi.org/10.1051/0004-6361/201937035 & © ESO 2020 Astrophysics The subsurface habitability of small, icy exomoons J. N. K. Y. Tjoa1,?, M. Mueller1,2,3, and F. F. S. van der Tak1,2 1 Kapteyn Astronomical Institute, University of Groningen, Landleven 12, 9747 AD Groningen, The Netherlands e-mail: [email protected] 2 SRON Netherlands Institute for Space Research, Landleven 12, 9747 AD Groningen, The Netherlands 3 Leiden Observatory, Leiden University, Niels Bohrweg 2, 2300 RA Leiden, The Netherlands Received 1 November 2019 / Accepted 8 March 2020 ABSTRACT Context. Assuming our Solar System as typical, exomoons may outnumber exoplanets. If their habitability fraction is similar, they would thus constitute the largest portion of habitable real estate in the Universe. Icy moons in our Solar System, such as Europa and Enceladus, have already been shown to possess liquid water, a prerequisite for life on Earth. Aims. We intend to investigate under what thermal and orbital circumstances small, icy moons may sustain subsurface oceans and thus be “subsurface habitable”. We pay specific attention to tidal heating, which may keep a moon liquid far beyond the conservative habitable zone. Methods. We made use of a phenomenological approach to tidal heating. We computed the orbit averaged flux from both stellar and planetary (both thermal and reflected stellar) illumination. We then calculated subsurface temperatures depending on illumination and thermal conduction to the surface through the ice shell and an insulating layer of regolith. We adopted a conduction only model, ignoring volcanism and ice shell convection as an outlet for internal heat. -
Margaret Kivelson
Margaret Galland Kivelson 6/27/2013 Margaret Kivelson- Dynamics - MoP 2011 – Boston University 1 Rotationally driven magnetospheres! (Mauk et al., (Saturn, Chapter 11) state: “while it is true that Saturn’s magnetosphere is intermediate between those of Earth and Jupiter in terms of size (whether measured by RP; RPP, or RMP), it is not intermediate in any meaningful dynamical sense. It is clearly rotationally driven like Jupiter’s, not solar-wind–driven like Earth’s.” Margaret Kivelson- Dynamics - MoP 6/27/2013 2011 – Boston University 2 This Vasyliunas (1983) diagram is a necessary element of any discussion of the magnetospheres of gas giants! It captures some critical features implicitly or explicitly: A significant source of heavy plasma deep within the magnetopause (Io, Enceladus) is spun up to some fraction of corotation speed by field-aligned currents coupling magnetosphere and ionosphere. Rotation dominates the dynamics – drives plasmoid releases down the tail. Solar wind shapes the boundaries but does not dominate the dynamics. Margaret Kivelson- Dynamics - MoP 6/27/2013 2011 – Boston University 3 Thomas et al., 2004 Schneider and Trager, 1995 In the pickup process, ions acquire perp. thermal speed of local rotation speed. 2 Energy added N pum() Pickup energy is shared with background plasma. Typically heats plasma. Melin6/27/2013 et al., 2009 4 Much is well established, but puzzles remain. Discuss a few features energy density of plasma and why it changes vs. radial distance, vs. local time, periodicities, Anomalies in regions of high dust density. Margaret Kivelson- Dynamics - MoP 6/27/2013 2011 – Boston University 5 At Earth, temperature (more correctly Below a plot from Kane et al (1995) thermal energy per particle) decreases of Voyager data at Jupiter, modeled with but not at Jupiter or Saturn. -
When the Net Force That Acts on a Hockey Puck Is 10 N, the Puck
Chapter 5 Circular Motion, the Planets, and Gravity Uniform Circular Motion Uniform circular motion is the. motion of an object traveling at a constant (uniform) speed in a circular path. • Because velocity is a vector, with a magnitude and direction, an object that is turning at a constant speed has a change in velocity. The object is accelerating. – If the object was not accelerating, it would be traveling at a constant speed in a straight line. – We will determine the magnitude and direction of the acceleration for an object moving at a constant speed in a circle Direction of Acceleration for Uniform Circular Motion. v Define an axis that is always tangential to the velocity (t), and an axis that is always perpendicular to that, radial (r), or centripetal (c). What would an acceleration in the tangential direction do? It must change the speed of the object. But for uniform circular motion, the speed doesn’t change, so the acceleration can not be tangential and must be radial. Consider a object that is twirled on a v1 string in a circle at a constant speed in a clockwise direction, as shown. Let’s P1 find the direction of the average P2 acceleration between points P1 and P2? v2 – v1 = Dv v1 + Dv = v2 v2 v This direction of Δv is the direction 1 of the acceleration. It is directly toward the center of the circle at the v2 Dv point midway between P1 and P2. The direction of acceleration is toward the center of the circle. It is called centripetal (center-seeking) acceleration. -
Arxiv:1508.00321V1 [Astro-Ph.EP] 3 Aug 2015 -11Bdps,Knoytee Mikl´Os
CHEOPS performance for exomoons: The detectability of exomoons by using optimal decision algorithm A. E. Simon1,2 Physikalisches Institut, Center for Space and Habitability, University of Berne, CH-3012 Bern, Sidlerstrasse 5 [email protected] Gy. M. Szab´o1 Gothard Astrophysical Observatory and Multidisciplinary Research Center of Lor´and E¨otv¨os University, H-9700 Szombathely, Szent Imre herceg u. 112. [email protected] L. L. Kiss3 Konkoly Observatory, Research Centre for Astronomy and Earth Sciences, Hungarian Academy of Sciences, H-1121 Budapest, Konkoly Thege. Mikl´os. ´ut 15-17. [email protected] A. Fortier Physikalisches Institut, Center for Space and Habitability, University of Berne, CH-3012 Bern, Sidlerstrasse 5 [email protected] and W. Benz arXiv:1508.00321v1 [astro-ph.EP] 3 Aug 2015 Physikalisches Institut, Center for Space and Habitability, University of Berne, CH-3012 Bern, Sidlerstrasse 5 [email protected] 1Konkoly Observatory, Research Centre for Astronomy and Earth Sciences, Hungarian Academy of Sciences, H-1121 Budapest, Konkoly Thege. Mikl´os. ´ut 15-17. 2Gothard Astrophysical Observatory and Multidisciplinary Research Center of Lor´and E¨otv¨os University, H-9700 Szombathely, Szent Imre herceg u. 112. 3Sydney Institute for Astronomy, School of Physics, University of Sydney, NSW 2006, Australia – 2 – ABSTRACT Many attempts have already been made for detecting exomoons around transit- ing exoplanets but the first confirmed discovery is still pending. The experience that have been gathered so far allow us to better optimize future space telescopes for this challenge, already during the development phase. In this paper we focus on the forth- coming CHaraterising ExOPlanet Satellite (CHEOPS),describing an optimized decision algorithm with step-by-step evaluation, and calculating the number of required transits for an exomoon detection for various planet-moon configurations that can be observ- able by CHEOPS. -
Moons in Orbit by Katie Clark
Name: ______________________________ Moons in Orbit by Katie Clark Did you know that other planets have moons, too? These moons are called satellites. A satellite is something that orbits, or moves around a planet. Some of these moons are small. Some of these moons are big. Some of them are really amazing! Mars is our closest neighbor who has a moon —in fact, Mars has two of them! Mars’ moons are named Phobos and Deimos. These moons are shaped like potatoes! Phobos gets closer to Mars each time it rotates around the planet. This means that one day it could crash into Mars! Jupiter has over sixty moons. Ganymede is the largest out of any of the planets’ moons. It is bigger than the planet Mercury! Another amazing moon is Io. It is full of volcanoes! Saturn has big rings around it. These rings are made of moons that broke apart, and still orbit the planet. Saturn has fifty-three moons! Uranus has a famous moon, too. Titania is known for earthquakes! Some of Titania’s fault lines are a thousand miles long! All together Uranus has twenty-seven moons. The planet Neptune was named after a god of the sea. Scientists named Neptune’s moons after other sea gods! Triton was the first moon of Neptune that scientists found. It rotates in a different direction from the planet. Neptune has thirteen moons. Mercury and Venus are the only two planets in our solar system that don’t have moons. They are so close to the sun that any moons would be pulled away by the sun’s gravity. -
Abstracts of the 50Th DDA Meeting (Boulder, CO)
Abstracts of the 50th DDA Meeting (Boulder, CO) American Astronomical Society June, 2019 100 — Dynamics on Asteroids break-up event around a Lagrange point. 100.01 — Simulations of a Synthetic Eurybates 100.02 — High-Fidelity Testing of Binary Asteroid Collisional Family Formation with Applications to 1999 KW4 Timothy Holt1; David Nesvorny2; Jonathan Horner1; Alex B. Davis1; Daniel Scheeres1 Rachel King1; Brad Carter1; Leigh Brookshaw1 1 Aerospace Engineering Sciences, University of Colorado Boulder 1 Centre for Astrophysics, University of Southern Queensland (Boulder, Colorado, United States) (Longmont, Colorado, United States) 2 Southwest Research Institute (Boulder, Connecticut, United The commonly accepted formation process for asym- States) metric binary asteroids is the spin up and eventual fission of rubble pile asteroids as proposed by Walsh, Of the six recognized collisional families in the Jo- Richardson and Michel (Walsh et al., Nature 2008) vian Trojan swarms, the Eurybates family is the and Scheeres (Scheeres, Icarus 2007). In this theory largest, with over 200 recognized members. Located a rubble pile asteroid is spun up by YORP until it around the Jovian L4 Lagrange point, librations of reaches a critical spin rate and experiences a mass the members make this family an interesting study shedding event forming a close, low-eccentricity in orbital dynamics. The Jovian Trojans are thought satellite. Further work by Jacobson and Scheeres to have been captured during an early period of in- used a planar, two-ellipsoid model to analyze the stability in the Solar system. The parent body of the evolutionary pathways of such a formation event family, 3548 Eurybates is one of the targets for the from the moment the bodies initially fission (Jacob- LUCY spacecraft, and our work will provide a dy- son and Scheeres, Icarus 2011). -
Planetary Magnetospheres
CLBE001-ESS2E November 9, 2006 17:4 100-C 25-C 50-C 75-C C+M 50-C+M C+Y 50-C+Y M+Y 50-M+Y 100-M 25-M 50-M 75-M 100-Y 25-Y 50-Y 75-Y 100-K 25-K 25-19-19 50-K 50-40-40 75-K 75-64-64 Planetary Magnetospheres Margaret Galland Kivelson University of California Los Angeles, California Fran Bagenal University of Colorado, Boulder Boulder, Colorado CHAPTER 28 1. What is a Magnetosphere? 5. Dynamics 2. Types of Magnetospheres 6. Interaction with Moons 3. Planetary Magnetic Fields 7. Conclusions 4. Magnetospheric Plasmas 1. What is a Magnetosphere? planet’s magnetic field. Moreover, unmagnetized planets in the flowing solar wind carve out cavities whose properties The term magnetosphere was coined by T. Gold in 1959 are sufficiently similar to those of true magnetospheres to al- to describe the region above the ionosphere in which the low us to include them in this discussion. Moons embedded magnetic field of the Earth controls the motions of charged in the flowing plasma of a planetary magnetosphere create particles. The magnetic field traps low-energy plasma and interaction regions resembling those that surround unmag- forms the Van Allen belts, torus-shaped regions in which netized planets. If a moon is sufficiently strongly magne- high-energy ions and electrons (tens of keV and higher) tized, it may carve out a true magnetosphere completely drift around the Earth. The control of charged particles by contained within the magnetosphere of the planet. -
A Jungian Interpretation of the Tempest
University of the Pacific Scholarly Commons University of the Pacific Theses and Dissertations Graduate School 1978 A Jungian interpretation of The Tempest Tana Smith University of the Pacific Follow this and additional works at: https://scholarlycommons.pacific.edu/uop_etds Part of the Literature in English, British Isles Commons Recommended Citation Smith, Tana. (1978). A Jungian interpretation of The Tempest. University of the Pacific, Thesis. https://scholarlycommons.pacific.edu/uop_etds/1989 This Thesis is brought to you for free and open access by the Graduate School at Scholarly Commons. It has been accepted for inclusion in University of the Pacific Theses and Dissertations by an authorized administrator of Scholarly Commons. For more information, please contact [email protected]. A JUNGil-..~~ INTERPllliTATION OF THE 'rEHPES'r by Tana Smit!1 An Essay Presented to the Faculty of the Graduate School Univers ity of the Pac ific In Pa rtial Fulfillment of the Requireme nts for the Degree Maste r of Arts Hay 1978 The following psychological interpretation of Shakespeare's 1 The Tempest is unique to articles on the ·same subject which have appeared in literary journals because it applies a purely Jungian reading to the characters in the play. Here each character is shown to represent one of the archetypes which Jung described in his book Archetypes ~ the Collective Unconscious. In giving the play a psychological interpretation, the action must be seen to occur inside Prospera's own unconscious mind. He is experiencing a psychic transformation or what Jung called the individuation process, where a person becomes "a separate, indivisible unity or 2 whole" and where the conscious and unconscious are united. -
Deep Space Chronicle Deep Space Chronicle: a Chronology of Deep Space and Planetary Probes, 1958–2000 | Asifa
dsc_cover (Converted)-1 8/6/02 10:33 AM Page 1 Deep Space Chronicle Deep Space Chronicle: A Chronology ofDeep Space and Planetary Probes, 1958–2000 |Asif A.Siddiqi National Aeronautics and Space Administration NASA SP-2002-4524 A Chronology of Deep Space and Planetary Probes 1958–2000 Asif A. Siddiqi NASA SP-2002-4524 Monographs in Aerospace History Number 24 dsc_cover (Converted)-1 8/6/02 10:33 AM Page 2 Cover photo: A montage of planetary images taken by Mariner 10, the Mars Global Surveyor Orbiter, Voyager 1, and Voyager 2, all managed by the Jet Propulsion Laboratory in Pasadena, California. Included (from top to bottom) are images of Mercury, Venus, Earth (and Moon), Mars, Jupiter, Saturn, Uranus, and Neptune. The inner planets (Mercury, Venus, Earth and its Moon, and Mars) and the outer planets (Jupiter, Saturn, Uranus, and Neptune) are roughly to scale to each other. NASA SP-2002-4524 Deep Space Chronicle A Chronology of Deep Space and Planetary Probes 1958–2000 ASIF A. SIDDIQI Monographs in Aerospace History Number 24 June 2002 National Aeronautics and Space Administration Office of External Relations NASA History Office Washington, DC 20546-0001 Library of Congress Cataloging-in-Publication Data Siddiqi, Asif A., 1966 Deep space chronicle: a chronology of deep space and planetary probes, 1958-2000 / by Asif A. Siddiqi. p.cm. – (Monographs in aerospace history; no. 24) (NASA SP; 2002-4524) Includes bibliographical references and index. 1. Space flight—History—20th century. I. Title. II. Series. III. NASA SP; 4524 TL 790.S53 2002 629.4’1’0904—dc21 2001044012 Table of Contents Foreword by Roger D.