Dawn at Ceres: What Have We Learned? J
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Formation of TRAPPIST-1
EPSC Abstracts Vol. 11, EPSC2017-265, 2017 European Planetary Science Congress 2017 EEuropeaPn PlanetarSy Science CCongress c Author(s) 2017 Formation of TRAPPIST-1 C.W Ormel, B. Liu and D. Schoonenberg University of Amsterdam, The Netherlands ([email protected]) Abstract start to drift by aerodynamical drag. However, this growth+drift occurs in an inside-out fashion, which We present a model for the formation of the recently- does not result in strong particle pileups needed to discovered TRAPPIST-1 planetary system. In our sce- trigger planetesimal formation by, e.g., the streaming nario planets form in the interior regions, by accre- instability [3]. (a) We propose that the H2O iceline (r 0.1 au for TRAPPIST-1) is the place where tion of mm to cm-size particles (pebbles) that drifted ice ≈ the local solids-to-gas ratio can reach 1, either by from the outer disk. This scenario has several ad- ∼ vantages: it connects to the observation that disks are condensation of the vapor [9] or by pileup of ice-free made up of pebbles, it is efficient, it explains why the (silicate) grains [2, 8]. Under these conditions plan- TRAPPIST-1 planets are Earth mass, and it provides etary embryos can form. (b) Due to type I migration, ∼ a rationale for the system’s architecture. embryos cross the iceline and enter the ice-free region. (c) There, silicate pebbles are smaller because of col- lisional fragmentation. Nevertheless, pebble accretion 1. Introduction remains efficient and growth is fast [6]. (d) At approx- TRAPPIST-1 is an M8 main-sequence star located at a imately Earth masses embryos reach their pebble iso- distance of 12 pc. -
News Feature: the Mars Anomaly
NEWS FEATURE NEWS FEATURE The Mars anomaly The red planet’s size is at the heart of a rift of ideas among researchers modeling the solar system’s formation. Stephen Ornes, Science Writer The presence of water isn’t the only Mars mystery sci- debate, data, and computer simulations, until re- entists are keen to probe. Another centers around a cently most models predicted that Mars should be seemingly trivial characteristic of the Red Planet: its many times its observed size. Getting Mars to form size. Classic models of solar system formation predict attherightplacewiththerightsizeisacrucialpartof that the girth of rocky worlds should grow with their any coherent explanation of the solar system’sevo- distance from the sun. Venus and Earth, for example, lution from a disk of gas and dust to its current con- should exceed Mercury, which they do. Mars should at figuration. In trying to do so, researchers have been — least match Earth, which it doesn’t. The diameter of the forced to devise models that are more detailed and — RedPlanetislittlemorethanhalfthatofEarth(1,2). even wilder than any seen before. “We still don’t understand why Mars is so small,” Nebulous Notions says astronomer Anders Johansen, who builds com- The solar system began as an immense cloud of dust putational models of planet formation at Lund Univer- and gas called a nebula. The idea of a nebular origin sity in Sweden. “It’s a really compelling question that dates back nearly 300 years. In 1734, Swedish scientist drives a lot of new theories.” and mystic Emanuel Swedenborg—whoalsoclaimed Understanding the planet’s diminutive size is key that Martian spirits had communed with him—posited to knowing how the entire solar system formed. -
Setting the Stage: Planet Formation and Volatile Delivery
Noname manuscript No. (will be inserted by the editor) Setting the Stage: Planet formation and Volatile Delivery Julia Venturini1 · Maria Paula Ronco2;3 · Octavio Miguel Guilera4;2;3 Received: date / Accepted: date Abstract The diversity in mass and composition of planetary atmospheres stems from the different building blocks present in protoplanetary discs and from the different physical and chemical processes that these experience during the planetary assembly and evolution. This review aims to summarise, in a nutshell, the key concepts and processes operating during planet formation, with a focus on the delivery of volatiles to the inner regions of the planetary system. 1 Protoplanetary discs: the birthplaces of planets Planets are formed as a byproduct of star formation. In star forming regions like the Orion Nebula or the Taurus Molecular Cloud, many discs are observed around young stars (Isella et al, 2009; Andrews et al, 2010, 2018a; Cieza et al, 2019). Discs form around new born stars as a natural consequence of the collapse of the molecular cloud, to conserve angular momentum. As in the interstellar medium, it is generally assumed that they contain typically 1% of their mass in the form of rocky or icy grains, known as dust; and 99% in the form of gas, which is basically H2 and He (see, e.g., Armitage, 2010). However, the dust-to-gas ratios are usually higher in discs (Ansdell et al, 2016). There is strong observational evidence supporting the fact that planets form within those discs (Bae et al, 2017; Dong et al, 2018; Teague et al, 2018; Pérez et al, 2019), which are accordingly called protoplanetary discs. -
Ahuna Mons on Ceres 29 July 2019
Image: Ahuna Mons on Ceres 29 July 2019 More recently, a study of Dawn data led by ESA research fellow Ottaviano Ruesch and Antonio Genova (Sapienza Università di Roma), published in Nature Geoscience in June, suggests that a briny, muddy 'slurry' exists below Ceres' surface, surging upwards towards and through the crust to create Ahuna Mons. Another recent study, led by Javier Ruiz of Universidad Complutense de Madrid and published in Nature Astronomy in July, also indicates that the dwarf planet has a surprisingly dynamic geology. Ceres was also the focus of an earlier study by Credit: NASA/JPL-Caltech/UCLA/MPS/DLR/IDA ESA's Herschel space observatory, which detected water vapour around the dwarf planet. Published in Nature in 2014, the result provided a strong indication that Ceres has ice on or near its surface. This image, based on observations from NASA's Dawn confirmed Ceres' icy crust via direct Dawn spacecraft, shows the largest mountain on observation in 2016, however, the contribution of the dwarf planet Ceres. the ice deposits to Ceres' exosphere turned out to be much lower than that inferred from the Herschel Dawn was the first mission to orbit an object in the observations. asteroid belt between Mars and Jupiter, and spent time at both large asteroid Vesta and dwarf planet The perspective view depicted in this image uses Ceres. Ceres is one of just five recognised dwarf enhanced-color combined images taken using blue planets in the Solar System (Pluto being another). (440 nm), green (750 nm), and infrared (960 nm) Dawn entered orbit around this rocky world on 6 filters, with a resolution of 35 m/pixel. -
The Formation of Jupiter by Hybrid Pebble-Planetesimal Accretion
The formation of Jupiter by hybrid pebble-planetesimal accretion Author: Yann Alibert1, Julia Venturini2, Ravit Helled2, Sareh Ataiee1, Remo Burn1, Luc Senecal1, Willy Benz1, Lucio Mayer2, Christoph Mordasini1, Sascha P. Quanz3, Maria Schönbächler4 Affiliations: 1Physikalisches Institut & Center for Space and Habitability, Universität Bern, Gesellschaftsstrasse 6, 3012 Bern, Switzerland 2Institut for Computational Sciences, Universität Zürich, Winterthurstrasse 190, 8057 Zürich, Switzerland 3 Institute for Particle Physics and Astrophysics, ETH Zürich, Wolfgang-Pauli-Strasse 27, 8093 Zürich, Switzerland 4Institute of Geochemistry and Petrology, ETH Zürich, Clausiusstrasse 25, 8092 Zürich, Switzerland The standard model for giant planet formation is based on the accretion of solids by a growing planetary embryo, followed by rapid gas accretion once the planet exceeds a so- called critical mass1. The dominant size of the accreted solids (cm-size particles named pebbles or km to hundred km-size bodies named planetesimals) is, however, unknown1,2. Recently, high-precision measurements of isotopes in meteorites provided evidence for the existence of two reservoirs in the early Solar System3. These reservoirs remained separated from ~1 until ~ 3 Myr after the beginning of the Solar System's formation. This separation | downloaded: 6.1.2020 is interpreted as resulting from Jupiter growing and becoming a barrier for material transport. In this framework, Jupiter reached ~20 Earth masses (M⊕) within ~1 Myr and 3 slowly grew to ~50 M⊕ in the subsequent 2 Myr before reaching its present-day mass . The evidence that Jupiter slowed down its growth after reaching 20 M⊕ for at least 2 Myr is puzzling because a planet of this mass is expected to trigger fast runaway gas accretion4,5. -
Planet Formation by Pebble Accretion in Ringed Disks A
A&A 638, A1 (2020) https://doi.org/10.1051/0004-6361/202037983 Astronomy & © A. Morbidelli 2020 Astrophysics Planet formation by pebble accretion in ringed disks A. Morbidelli Département Lagrange, University of Nice – Sophia Antipolis, CNRS, Observatoire de la Côte d’Azur, Nice, France e-mail: [email protected] Received 19 March 2020 / Accepted 9 April 2020 ABSTRACT Context. Pebble accretion is expected to be the dominant process for the formation of massive solid planets, such as the cores of giant planets and super-Earths. So far, this process has been studied under the assumption that dust coagulates and drifts throughout the full protoplanetary disk. However, observations show that many disks are structured in rings that may be due to pressure maxima, preventing the global radial drift of the dust. Aims. We aim to study how the pebble-accretion paradigm changes if the dust is confined in a ring. Methods. Our approach is mostly analytic. We derived a formula that provides an upper bound to the growth of a planet as a function of time. We also numerically implemented the analytic formulæ to compute the growth of a planet located in a typical ring observed in the DSHARP survey, as well as in a putative ring rescaled at 5 AU. Results. Planet Type I migration is stopped in a ring, but not necessarily at its center. If the entropy-driven corotation torque is desaturated, the planet is located in a region with low dust density, which severely limits its accretion rate. If the planet is instead near the ring’s center, its accretion rate can be similar to the one it would have in a classic (ringless) disk of equivalent dust density. -
POSTER SESSION I: CERES: MISSION RESULTS from DAWN 6:00 P.M
Lunar and Planetary Science XLVIII (2017) sess312.pdf Tuesday, March 21, 2017 [T312] POSTER SESSION I: CERES: MISSION RESULTS FROM DAWN 6: 00 p.m. Town Center Exhibit Area Russell C. T. Raymond C. A. De Sanctis M. C. Nathues A. Prettyman T. H. et al. POSTER LOCATION #171 Dawn at Ceres: What We Have Learned [#1269] A summary of the major discoveries and their implications at the close of the exploration of Ceres by Dawn. Ermakov A. I. Park R. S. Zuber M. T. Smith D. E. Fu R. R. et al. POSTER LOCATION #172 Regional Analysis of Ceres’ Gravity Anomalies [#1374] Put in geological and geomorphological context, the regional gravity anomalies give clues on the structure and evolution of Ceres’ crust. Nathues A. Platz T. Thangjam G. Hoffmann M. Mengel K. et al. POSTER LOCATION #173 Evolution of Occator Crater on (1) Ceres [#1385] We present recent results on the origin and evolution of the bright spots (Cerealia and Vinalia Faculae) at crater Occator on (1) Ceres. Buczkowski D. L. Scully J. E. C. Schenk P. M. Ruesch O. von der Gathen I. et al. POSTER LOCATION #174 Tectonic Analysis of Fracturing Associated with Occator Crater [#1488] The floor, walls, and ejecta of Occator Crater on Ceres are cut by multiple sets of linear and concentric fractures. We explore possible formation mechanisms. Pasckert J. H. Hiesinger H. Raymond C. A. Russell C. POSTER LOCATION #175 Degradation and Ejecta Mobility of Impact Craters on Ceres [#1377] We investigated the degradation and ejecta mobility of craters on Ceres, to investigate latitudinal variations, and to compare it with other planetary bodies. -
New Studies Provide Unexpected Insights Into Dwarf Planet Ceres 1 September 2016
New studies provide unexpected insights into dwarf planet Ceres 1 September 2016 Mons. The dome-shaped mountain has an elliptical base and a concave top, as well as other properties that indicate cryovolcanism. The authors applied models to determine the age of Ahuna Mons, finding it to have formed after the craters surrounding it, which suggests that it came into existence relatively recently. There is no evidence for compressional tectonism, nor for erosional features, the authors say; it appears that extrusion is a main driver behind the formation of Ahuna Mons. Although the exact material driving the cryovolcano cannot be determined without further data, the authors propose that chlorine salts, which have been previously detected in a different region of Ceres, could have been present with water ice below Ceres' surface and driven the chemical activity that formed Ahuna Mons. In a second study, Jean-Philippe Combe et al. A high resolution Dawn framing camera image of Ahuna describe the detection of water ice - exposed on the Mons. Image width is 30 km. Credit: NASA/JPL- surface of Ceres. The dwarf planet was known to Caltech/UCLA/MPS/DLR/IDA contain water ice, but water ice is also expected to be unstable on its surface, so scientists were unsure whether it could be detected there. They used the Visible and InfraRed (VIR) mapping Six studies published today in Science highlight spectrometer onboard the Dawn spacecraft to new and unexpected insights into Ceres, a dwarf analyze a highly reflective zone in a young crater planet and the largest object in the asteroid belt called Oxo, on five occasions during 2015. -
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, -
16. Ice in the Martian Regolith
16. ICE IN THE MARTIAN REGOLITH S. W. SQUYRES Cornell University S. M. CLIFFORD Lunar and Planetary Institute R. O. KUZMIN V.I. Vernadsky Institute J. R. ZIMBELMAN Smithsonian Institution and F. M. COSTARD Laboratoire de Geographie Physique Geologic evidence indicates that the Martian surface has been substantially modified by the action of liquid water, and that much of that water still resides beneath the surface as ground ice. The pore volume of the Martian regolith is substantial, and a large amount of this volume can be expected to be at tem- peratures cold enough for ice to be present. Calculations of the thermodynamic stability of ground ice on Mars suggest that it can exist very close to the surface at high latitudes, but can persist only at substantial depths near the equator. Impact craters with distinctive lobale ejecta deposits are common on Mars. These rampart craters apparently owe their morphology to fluidhation of sub- surface materials, perhaps by the melting of ground ice, during impact events. If this interpretation is correct, then the size frequency distribution of rampart 523 524 S. W. SQUYRES ET AL. craters is broadly consistent with the depth distribution of ice inferred from stability calculations. A variety of observed Martian landforms can be attrib- uted to creep of the Martian regolith abetted by deformation of ground ice. Global mapping of creep features also supports the idea that ice is present in near-surface materials at latitudes higher than ± 30°, and suggests that ice is largely absent from such materials at lower latitudes. Other morphologic fea- tures on Mars that may result from the present or former existence of ground ice include chaotic terrain, thermokarst and patterned ground. -
Oxo Crater on (1) Ceres: Geological History and the Role of Water-Ice
The Astronomical Journal, 154:84 (13pp), 2017 September https://doi.org/10.3847/1538-3881/aa7a04 © 2017. The American Astronomical Society. All rights reserved. Oxo Crater on (1) Ceres: Geological History and the Role of Water-ice A. Nathues1, T. Platz1, M. Hoffmann1, G. Thangjam1, E. A. Cloutis2, D. M. Applin2, L. Le Corre1,3, V. Reddy1,4, K. Mengel5, S. Protopapa6, D. Takir7, F. Preusker8, B. E. Schmidt9, and C. T. Russell10 1 Max Planck Institute for Solar System Research, Justus-von-Liebig-Weg 3, D-37077 Goettingen, Germany; [email protected] 2 University of Winnipeg, Winnipeg, MB R3B 2E9, Canada 3 Planetary Science Institute, 1700 East Fort Lowell Rd, Suite 106, Tucson, AZ 85719-2395, USA 4 Lunar and Planetary Laboratory, University of Arizona, Tucson, AZ, USA 5 IELF, TU Clausthal, Adolph-Roemer-Straße 2A, D-38678 Clausthal-Zellerfeld, Germany 6 University of Maryland, Department of Astronomy, College Park, MD 20742, USA 7 SETI Institute, Mountain View, CA 94043, USA 8 German Aerospace Center (DLR), Institute of Planetary Research, D-12489 Berlin, Germany 9 Georgia Institute of Technology, Atlanta, GA, USA 10 Institute of Geophysics and Planetary Physics, Dept. of Earth, Planetary and Space Sciences, University of California Los Angeles, Los Angeles, CA, USA Received 2017 March 1; revised 2017 June 14; accepted 2017 June 14; published 2017 August 4 Abstract Dwarf planet Ceres (∅∼940 km) is the largest object in the main asteroid belt. Investigations suggest that Ceres is a thermally evolved, volatile-rich body with potential geological activity, a body that was never completely molten, but one that possibly partially differentiated into a rocky core and an ice-rich mantle, and may contain remnant internal liquid water. -
Surface Residence Times of Regolith on the Lunar Maria
52nd Lunar and Planetary Science Conference 2021 (LPI Contrib. No. 2548) 1652.pdf 1 1 SURFACE RESIDENCE TIMES OF REGOLITH ON THE LUNAR MARIA. P. O’Brien and S. Byrne , 1 L unar and Planetary Laboratory, University of Arizona, Tucson, AZ 85721 ([email protected]) Introduction: The surfaces of airless bodies like Our model simulates mare-like surfaces evolving the Moon undergo microscopic chemical changes as a over time from flat surfaces to cratered landscapes. result of energetic processes operating in the space Impacts are randomly sampled from the present-day environment, collectively known as space weathering lunar impact flux [5] and the global population of [1,2]. Despite returned lunar soil samples, the rate of secondary craters produced by these impacts is space weathering on the Moon is not well understood. generated following empirical observations of The amount of chemical weathering incurred in the secondary production on airless bodies [6,7]. At each lunar regolith depends critically on the rate at which timestep, we compute the downslope flux of regolith regolith is excavated, transported, and buried by by solving the 2D diffusion equation [8]. The rate of macroscopic impact processes. These physical diffusion is calibrated by matching the average processes control how long regolith spends on the roughness of the model landscapes to the observed surface where it is exposed to the space environment. roughness of the lunar maria, as measured by the We have developed a Monte Carlo model that median bidirectional slope at 4 m baselines [9]. Figure simulates the evolution of lunar maria landscapes 1 shows how model surfaces subject to these physical under topographic relief-creation from impact cratering processes become rougher and more heavily-cratered and relief-reduction from micrometeorite gardening over time.