Ceres' Partial Differentiation: Undifferentiated Crust Mixing with A
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
A Possible Explanation of the Secular Increase of the Astronomical Unit 1
T. Miura 1 A possible explanation of the secular increase of the astronomical unit Takaho Miura(a), Hideki Arakida, (b) Masumi Kasai(a) and Syuichi Kuramata(a) (a)Faculty of Science and Technology,Hirosaki University, 3 bunkyo-cyo Hirosaki, Aomori, 036-8561, Japan (b)Education and integrate science academy, Waseda University,1 waseda sinjuku Tokyo, Japan Abstract We give an idea and the order-of-magnitude estimations to explain the recently re- ported secular increase of the Astronomical Unit (AU) by Krasinsky and Brumberg (2004). The idea proposed is analogous to the tidal acceleration in the Earth-Moon system, which is based on the conservation of the total angular momentum and we apply this scenario to the Sun-planets system. Assuming the existence of some tidal interactions that transfer the rotational angular momentum of the Sun and using re- d ported value of the positive secular trend in the astronomical unit, dt 15 4(m/s),the suggested change in the period of rotation of the Sun is about 21(ms/cy) in the case that the orbits of the eight planets have the same "expansionrate."This value is suf- ficiently small, and at present it seems there are no observational data which exclude this possibility. Effects of the change in the Sun's moment of inertia is also investi- gated. It is pointed out that the change in the moment of inertia due to the radiative mass loss by the Sun may be responsible for the secular increase of AU, if the orbital "expansion"is happening only in the inner planets system. -
March 21–25, 2016
FORTY-SEVENTH LUNAR AND PLANETARY SCIENCE CONFERENCE PROGRAM OF TECHNICAL SESSIONS MARCH 21–25, 2016 The Woodlands Waterway Marriott Hotel and Convention Center The Woodlands, Texas INSTITUTIONAL SUPPORT Universities Space Research Association Lunar and Planetary Institute National Aeronautics and Space Administration CONFERENCE CO-CHAIRS Stephen Mackwell, Lunar and Planetary Institute Eileen Stansbery, NASA Johnson Space Center PROGRAM COMMITTEE CHAIRS David Draper, NASA Johnson Space Center Walter Kiefer, Lunar and Planetary Institute PROGRAM COMMITTEE P. Doug Archer, NASA Johnson Space Center Nicolas LeCorvec, Lunar and Planetary Institute Katherine Bermingham, University of Maryland Yo Matsubara, Smithsonian Institute Janice Bishop, SETI and NASA Ames Research Center Francis McCubbin, NASA Johnson Space Center Jeremy Boyce, University of California, Los Angeles Andrew Needham, Carnegie Institution of Washington Lisa Danielson, NASA Johnson Space Center Lan-Anh Nguyen, NASA Johnson Space Center Deepak Dhingra, University of Idaho Paul Niles, NASA Johnson Space Center Stephen Elardo, Carnegie Institution of Washington Dorothy Oehler, NASA Johnson Space Center Marc Fries, NASA Johnson Space Center D. Alex Patthoff, Jet Propulsion Laboratory Cyrena Goodrich, Lunar and Planetary Institute Elizabeth Rampe, Aerodyne Industries, Jacobs JETS at John Gruener, NASA Johnson Space Center NASA Johnson Space Center Justin Hagerty, U.S. Geological Survey Carol Raymond, Jet Propulsion Laboratory Lindsay Hays, Jet Propulsion Laboratory Paul Schenk, -
Fracture Geometry and Statistics of Ceres' Floor Fractures
1 Fracture Geometry and Statistics of Ceres’ Floor Fractures 2 3 K. Krohn1, D. L. Buczkowski2, I. von der Gathen1, R. Jaumann1,3, F. Schulzeck1, K. Stephan1, R. 4 Wagner1, J. E. C. Scully4, C. A. Raymond4, C. T. Russell5 5 6 1Institute of Planetary Research, German Aerospace Center, Berlin, Germany; 2Johns Hopkins 7 University Applied Physics Laboratory, Laurel, MD, USA; 3Freie Universiät Berlin, Germany; 8 4NASA JPL, California Institute of Technology, Pasadena, California, USA; 5UCLA, Institute of 9 Geophysics, Los Angeles, CA, USA 10 11 Corresponding author: Katrin Krohn, [email protected], Rutherfordstraße 2, 12489 Berlin, Germany 12 13 Keywords: Ceres, dwarf planet, floor fractured craters 14 15 16 Highlights: 17 18 We measured 2336 fractures in thirteen floor-fractured craters (FFC) on Ceres. 19 20 Floor-fractured craters on Ceres share similarities with FFCs on other planetary bodies 21 especially those on the Moon and Mars. 22 23 On Ceres some floor-fractured craters are impact-driven; other appear to be related to cooling- 24 melting processes, outgassing and/or tectonics such as doming of the subsurface. 25 26 Fracture studies point out brittle surface materials. 27 28 29 30 Abstract 31 32 Floor-fractured craters are one of the most distinct features on Ceres. Most of the fractures are located 33 on the crater floors. The floor-fractures are concentric, radial or polygonal and share similarities with 34 Class 1 and 4 floor-fractured craters (FFC) on the Moon (e.g., Buczkowski et al., 2018; Schultz, 1976) 35 In total we measured 2336 fractures in thirteen craters. -
Planetary Seismology
This article was originally published in Treatise on Geophysics, Second Edition, published by Elsevier, and the attached copy is provided by Elsevier for the author's benefit and for the benefit of the author's institution, for non-commercial research and educational use including without limitation use in instruction at your institution, sending it to specific colleagues who you know, and providing a copy to your institution’s administrator. All other uses, reproduction and distribution, including without limitation commercial reprints, selling or licensing copies or access, or posting on open internet sites, your personal or institution’s website or repository, are prohibited. For exceptions, permission may be sought for such use through Elsevier's permissions site at: http://www.elsevier.com/locate/permissionusematerial Lognonné P., and Johnson C.L Planetary Seismology. In: Gerald Schubert (editor-in- chief) Treatise on Geophysics, 2nd edition, Vol 10. Oxford: Elsevier; 2015. p. 65-120. Author's personal copy 10.03 Planetary Seismology P Lognonne´, Universite´ Paris Diderot -Sorbonne Paris Cite´, Institut de Physique du Globe de Paris, Paris, France CL Johnson, University of British Columbia, Vancouver, BC, Canada; Planetary Science Institute, Tucson, AZ, USA ã 2015 Elsevier B.V. All rights reserved. 10.03.1 Introduction 65 10.03.2 Lunar Results 70 10.03.2.1 The Apollo PSE Data 70 10.03.2.2 Seismic-Velocity Structure: Crust and Mantle 72 10.03.2.3 Very Deep Interior 77 10.03.2.4 Mineralogical and Thermal Interpretation of Lunar Seismic -
DENSITY of the MANTLE of MARS Kenneth A. Goettel, Dept. of Earth and Planetary Sciences, Mcdonnell Center for the Space Sciences, Washington, University, St
DENSITY OF THE MANTLE OF MARS Kenneth A. Goettel, Dept. of Earth and Planetary Sciences, McDonnell Center for the Space Sciences, Washington, University, St. Louis, MO 63130 The zero pressure density of the Martian mantle is an important constraint on the composition and mineralogy of the mantle. The mean density and moment of inertia factor of Mars constrain the density of the Martian mantle, but do not define it uniquely. The mean density of Mars, 3.933+0.002 g/cm3 (1) is well determined. The estimated moment of inertia factor wFich Mars would have if Mars were in hydrostatic equilibrium, 0.365 (2,3), may still be significantly model dependent. With these constraints, the estimated zero pressure density of the Martian mantle varies as a function of the core composition assumed and as a function of the elastic data chosen as represent- ative of the Martian interior. Recent estimates of the zero pressure density of the Martian mantle are shown in Table 1. The results of Johnston et a1 . (4) were based on a value of 0.377 for the moment of inertia factor of Mars. The results of Johnston and ToksBz (5) and Okal and Anderson (6) were both based on the revised (2,3) value of 0.365 for the moment of inertia factor. The results of (5) and (6) are not completely comparable, since (5) did not give the densities assumed for their core compositions, and (6) did not give compositions corresponding to their core densities. Part of the motivation for the present work was to explore the reasons for the differences between the results of (5) and (6). -
Interior Structure of Terrestrial Planets Tilman Spohn Überblick Überblick Komplexe Systeme Weltraum
Interior Structure of Terrestrial Planets Tilman Spohn Überblick Überblick Komplexe Systeme Weltraum ErosionErosion durchdurch Sonnenwind;Sonnenwind; ImpakteImpakte Biosphäre Hydrosphäre Atmosphäre Kruste Biogeochemiche Wechselwirkungen stabilisieren die VulkanismusVulkanismus AusgasenAusgasen Oberflächentemperatur (Kohlenstoff Zyklus) Mantel Weltraum Magnetosphäre ErosionErosion durchdurch AbschiirmungAbschiirmung Sonnenwind;Sonnenwind; ImpakteImpakte Biosphäre Hydrosphäre Atmosphäre Kruste Subduktion,Subduktion, VolatilrückführungVolatilrückführung undund VulkanismusVulkanismus AusgasenAusgasen verstärkteverstärkte KühlungKühlung Mantel KonvektiveKonvektive KühlungKühlung Kern DynamoDynamo Die Allianz Interior Structure 7 Tilman Spohn, IfP Münster 0.5 ME 0.8 ME 1 ME 2.5 ME 5 ME Interior Structure Interior Structure models aim at determining Mars the masses of major chemical reservoirs the depths to chemical discontinuities and phase transition boundaries the variation with depth of thermodynamic state variables (r, P, T) and transport parameters Folie 9 > Spohn Of Particular Interest… Core radius State of the core Inner core radius Heat flow from the core Transport parameters Folie 10 > Spohn Interior Structure Constraints Mass Moment of inertia factor Gravity field, Topography Rotation parameters Tides Surface rock chemistry/ mineralogy Cosmochemical constraints Laboratory data Magnetism MGS Gravity Field of Mars Future: Seismology! Heat flow Folie 11 > Spohn Doppler Principle 12 T. Spohn, IfP June 24, 2003 Mars Jupiter Ganymede Chemical Components: Gas (H, He), Ice (NH3, CH4, H2O), Rock/Iron 13 Page 14 > Objectives and Accomplishments > Prof. Dr.Tilman Spohn Chemistry Chondritic ratio Fe/Si = 1.71 Mg2SiO4 (olivine) mantle and Fe core 16 Surface Rock 17 SNC Meteorites Samples from Mars? SNC: Shergotty,Nahkla, Chassigny Most of them are young: a few 100 million to 1 billion years Basalts 18 Tilman Spohn, IfP Münster 1st HGF Alliance Week, Berlin,14 May 2008 Dynamic Tidal Response Constraint Tidal deformation is characterized by .. -
Results from the NASA Dawn Mission to Vesta and Ceres
EPSC Abstracts Vol. 13, EPSC-DPS2019-5-1, 2019 EPSC-DPS Joint Meeting 2019 c Author(s) 2019. CC Attribution 4.0 license. The Geologic Mapping of Small Bodies: Results from the NASA Dawn Mission to Vesta and Ceres Williams, David A. and the Dawn Science Team School of Earth and Space Exploration, Arizona State University, Tempe, Arizona, USA, ([email protected]) Abstract 2. Ceres mapping & chronostratigraphy NASA’s Dawn mission was a Discovery-class robotic mission to send an orbiter to the two most massive The geologic mapping of Ceres was described in [5] objects in the Main Asteroid Belt, asteroid (4) Vesta and its chronostratigraphy is still being finalized at the and dwarf planet (1) Ceres [1]. Dawn orbited Vesta time of this writing. Ceres has a globally distributed from July 2011 to September 2012, and it remains in cratered terrain, with three large, ill-defined orbit of Ceres since it arrived in March 2015. As part topographic depressions that could be ancient basins. of the spacecraft’s nominal mission, the Dawn Science Kerwan crater (285 km diameter) is the largest Team requested geologic mapping campaigns of both identifiable impact crater, infilled and surrounded by Vesta and Ceres, which included global mapping a unique smooth material that marks this oldest crater. using High Altitude Mapping Orbit (HAMO) images In the southeastern hemisphere Yalode and Urvara (Vesta: 70 m/px; Ceres: 140 m/px) and quadrangle craters mark the next two youngest basins, with mapping using Low Altitude Mapping Orbit (LAMO) complex ejecta units. Intermediate and younger aged images (Vesta: 25/m/px; Ceres: 35 m/px). -
Enceladus: Present Internal Structure and Differentiation by Early and Long-Term Radiogenic Heating
Icarus 188 (2007) 345–355 www.elsevier.com/locate/icarus Enceladus: Present internal structure and differentiation by early and long-term radiogenic heating Gerald Schubert a,b,∗, John D. Anderson c,BryanJ.Travisd, Jennifer Palguta a a Department of Earth and Space Sciences, University of California, 595 Charles E. Young Drive East, Los Angeles, CA 90095-1567, USA b Institute of Geophysics and Planetary Physics, University of California, 603 Charles E. Young Drive East, Los Angeles, CA 90095-1567, USA c Global Aerospace Corporation, 711 West Woodbury Road, Suite H, Altadena, CA 91001-5327, USA d Earth & Environmental Sciences Division, EES-2/MS-F665, Los Alamos National Laboratory, Los Alamos, NM 87545, USA Received 30 May 2006; revised 27 November 2006 Available online 8 January 2007 Abstract Pre-Cassini images of Saturn’s small icy moon Enceladus provided the first indication that this satellite has undergone extensive resurfacing and tectonism. Data returned by the Cassini spacecraft have proven Enceladus to be one of the most geologically dynamic bodies in the Solar System. Given that the diameter of Enceladus is only about 500 km, this is a surprising discovery and has made Enceladus an object of much interest. Determining Enceladus’ interior structure is key to understanding its current activity. Here we use the mean density of Enceladus (as determined by the Cassini mission to Saturn), Cassini observations of endogenic activity on Enceladus, and numerical simulations of Enceladus’ thermal evolution to infer that this satellite is most likely a differentiated body with a large rock-metal core of radius about 150 to 170 km surrounded by a liquid water–ice shell. -
Geology of Dwarf Planet Ceres and Meteorite Analogs H
80th Annual Meeting of the Meteoritical Society 2017 (LPI Contrib. No. 1987) 6003.pdf GEOLOGY OF DWARF PLANET CERES AND METEORITE ANALOGS H. Y. McSween1, C. A. Raymond2, T. H. Prettyman3, M. C. De Sanctis4, J. C. Castillo-Rogez2, C. T. Russell5, and the Dawn Science Team, 1Department of Earth & Planetary Sciences, University of Tennessee, Knoxville, TN 37996-1410, [email protected]. 2Jet Propulsion Laboratory, Pasadena, CA 91109, 3Planetary Science Institute, Tucson, AZ 85719, 4Istituto di Astrofisica e Planetologia Spaziali, Istituto Nazionale di Astrofisica, Rome, Italy, 5Department of Earth, Planetary and Space Sciences, University of California, Los Angeles, CA 90095. Introduction: Although no known meteorites are thought to derive from Ceres, CI/CM carbonaceous chondrites are potential analogs for its composition and alteration [1]. These meteorites have primitive chemical compositions, despite having suffered aqueous alteration; this paradox can be explained by closed-system alteration in small parent bodies where low permeability limited fluid transport. In contrast, Ceres, the largest asteroidal body, has experi- enced extensive alteration accompanied by differentiation of silicates and volatiles [2]. The ancient surface of Ceres has a crater density similar to Vesta, but basins >400 km are absent or relaxed. The Dawn spacecraft’s GRaND instrument revealed near-surface ice concentrations in the regolith at high latitudes [3], exposed on the surface locally in a few craters [4]. The VIR instrument indicates a dark surface interpreted as a lag deposit from ice sublimation and composed of ammoniated clays, serpentine, MgCa-carbonates, and a darkening component [5]. Elemental analysis of Fe and H abundances in the non-icy regolith are lower and higher, respective- ly, than for CI/CM chondrites [3]. -
The Moment of Inertia Factor of Mars: Implications for Geochemical Models of the Mar- Tian Interior
Lunar and Planetary Science XXVIII 1147.PDF The Moment of Inertia Factor of Mars: Implications for Geochemical Models of the Mar- tian Interior. C.M. Bertka and Y. Fei, Geophysical Laboratory and Center for High-Pressure Re- search, Carnegie Institution of Washington, 5251 Broad Branch Rd., N.W., Washington DC 20015 (e-mail: [email protected]) Introduction: Data constraining the Results: The Dreibus and Wänke model structure and composition of the Martian in- predicts a core composition of Fe with terior are limited. Presently, the strongest 14 wt% S. The moment of inertia factor that geophysical constraint we have for Mars is we calculate for a DW model mantle and core knowledge of the mass and radius of the is 0.368. This calculation assumes a high- planet. Using the mass and radius of the temperature P-T profile for the Martian inte- planet and the moment of inertia factor as rior and does not include a crust. Choosing a constraints, two of three variables, mantle low-temperature profile for the interior results density, core size, and core density, can be in an increase of the moment of inertia factor calculated as a function of one of the three of 0.001. We have also considered a variation variables. Unfortunately, the Martian moment in core composition from pure Fe to FeS. This of inertia factor is not well known either. Bills variation results in a corresponding variation (1) has argued that the commonly accepted in core size, core size increases with increas- moment of inertia factor of 0.365 may be too ing S content, but changes the moment of in- high and that lower values are equally feasi- ertia factor by only ± 0.001. -
CORELESS TERRESTRIAL EXOPLANETS Linda T
The Astrophysical Journal, 688:628Y635, 2008 November 20 A # 2008. The American Astronomical Society. All rights reserved. Printed in U.S.A. CORELESS TERRESTRIAL EXOPLANETS Linda T. Elkins-Tanton Department Earth, Atmospheric, and Planetary Sciences, MIT, Building 54-824, 77 Massachusetts Avenue, Cambridge MA 02139; [email protected] and Sara Seager Department Earth, Atmospheric, and Planetary Sciences, Department of Physics, MIT, Building 54-1626, 77 Massachusetts Avenue, Cambridge MA 02139 Received 2008 March 8; accepted 2008 July 26 ABSTRACT Differentiation in terrestrial planets is expected to include the formation of a metallic iron core. We predict the existence of terrestrial planets that have differentiated but have no metallic core, planets that are effectively a giant silicate mantle. We discuss two paths to forming a coreless terrestrial planet, whereby the oxidation state during planetary accretion and solidification will determine the size or existence of any metallic core. Under this hypothesis, any metallic iron in the bulk accreting material is oxidized by water, binding the iron in the form of iron oxide into the silicate minerals of the planetary mantle. The existence of such silicate planets has consequences for interpreting the compositions and interior density structures of exoplanets based on their mass and radius measurements. Subject headinggs: accretion, accretion disks — planets and satellites: formation — solar system: formation Online material: color figure 1. INTRODUCTION the planet as well (Rubie et al. 2003; Terasaki et al. 2005; Jacobsen 2005). Heat is converted from the kinetic energy of Understanding the interior composition of exoplanets based on accretion and from potential energy release during differentiation. their mass and radius measurements is a growing field of study. -
Evidence for the Interior Evolution of Ceres from Geologic Analysis of Fractures
PUBLICATIONS Geophysical Research Letters RESEARCH LETTER Evidence for the Interior Evolution of Ceres 10.1002/2017GL075086 from Geologic Analysis of Fractures Key Points: J. E. C. Scully1 , D. L. Buczkowski2 , N. Schmedemann3 , C. A. Raymond1 , J. C. Castillo-Rogez1, • ≥ We identify all 1 km wide linear 4 5 1 ’ 6 7 8 features outside impact craters: most S. D. King , M. T. Bland , A. I. Ermakov ,D.P.OBrien , S. Marchi , A. Longobardo , 9 10 11 are secondary crater chains and there C. T. Russell ,R.R.Fu , and M. Neveu is one set of pit chains • Pit chains are the surface expression of 1Jet Propulsion Laboratory, California Institute of Technology, Pasadena, CA, USA, 2The Johns Hopkins University subsurface fractures, and they reveal Applied Physics Laboratory, Laurel, MD, USA, 3Institute of Geological Sciences, Freie Universität Berlin, Berlin, Germany, that the localized outer layer is thicker 4 5 ’ Department of Geosciences, Virginia Polytechnic Institute and State University, Blacksburg, VA, USA, U.S. Geological than Ceres s average 6 7 • We propose that a region of upwelling Survey, Astrogeology Science Center, Flagstaff, AZ, USA, Planetary Science Institute, Tucson, AZ, USA, Southwest Research 8 9 material, resulting from convection/ Institute, Boulder, CO, USA, INAF Istituto di Astrofisica e Planetologia Spaziali (IAPS), Rome, Italy, Department of Earth, diapirism, formed the pit chains, and Planetary, and Space Science, University of California, Los Angeles, CA, USA, 10Lamont-Doherty Earth Observatory, we derive its characteristics Columbia University, Palisades, NY, USA, 11School of Earth and Space Exploration, Arizona State University, Tempe, AZ, USA Supporting Information: • Supporting Information S1 Abstract Ceres is the largest asteroid belt object, and the Dawn spacecraft observed Ceres since 2015.