Science Case for a Lander Or Rover Mission to a Lunar Magnetic Anomaly and Swirl
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A Wunda-Full World? Carbon Dioxide Ice Deposits on Umbriel and Other Uranian Moons
Icarus 290 (2017) 1–13 Contents lists available at ScienceDirect Icarus journal homepage: www.elsevier.com/locate/icarus A Wunda-full world? Carbon dioxide ice deposits on Umbriel and other Uranian moons ∗ Michael M. Sori , Jonathan Bapst, Ali M. Bramson, Shane Byrne, Margaret E. Landis Lunar and Planetary Laboratory, University of Arizona, Tucson, AZ 85721, USA a r t i c l e i n f o a b s t r a c t Article history: Carbon dioxide has been detected on the trailing hemispheres of several Uranian satellites, but the exact Received 22 June 2016 nature and distribution of the molecules remain unknown. One such satellite, Umbriel, has a prominent Revised 28 January 2017 high albedo annulus-shaped feature within the 131-km-diameter impact crater Wunda. We hypothesize Accepted 28 February 2017 that this feature is a solid deposit of CO ice. We combine thermal and ballistic transport modeling to Available online 2 March 2017 2 study the evolution of CO 2 molecules on the surface of Umbriel, a high-obliquity ( ∼98 °) body. Consid- ering processes such as sublimation and Jeans escape, we find that CO 2 ice migrates to low latitudes on geologically short (100s–1000 s of years) timescales. Crater morphology and location create a local cold trap inside Wunda, and the slopes of crater walls and a central peak explain the deposit’s annular shape. The high albedo and thermal inertia of CO 2 ice relative to regolith allows deposits 15-m-thick or greater to be stable over the age of the solar system. -
General Disclaimer One Or More of the Following Statements May Affect
General Disclaimer One or more of the Following Statements may affect this Document This document has been reproduced from the best copy furnished by the organizational source. It is being released in the interest of making available as much information as possible. This document may contain data, which exceeds the sheet parameters. It was furnished in this condition by the organizational source and is the best copy available. This document may contain tone-on-tone or color graphs, charts and/or pictures, which have been reproduced in black and white. This document is paginated as submitted by the original source. Portions of this document are not fully legible due to the historical nature of some of the material. However, it is the best reproduction available from the original submission. Produced by the NASA Center for Aerospace Information (CASI) ^i e I !emote sousing sad eeolegio Studies of the llaistary Crusts Bernard Ray Hawke Prince-1 Investigator a EL r Z^ .99 University of Hawaii Hawaii Institute of Geophysics Planetary Geosciences Division Honolulu, Hawaii 96822 ^y 1i i W. December 1983 (NASA —CR-173215) REMOTE SENSING AND N84-17092 GEOLOGIC STUDIES OF THE PLANETARY CRUSTS Final Report ( Hawaii Inst. of Geophysics) 14 p HC A02/MF 101 CSCL 03B Unclas G3/91 11715 Gy -2- ©R1GNAL OF POOR QUALITY Table of Contents Page I. Remote Sensing and Geologic Studies cf Volcanic Deposits . • . 3 A. Spectral reflectance studies of dark-haloed craters. • . 3 B. Remote s^:sing studies of regions which were sites of ancient volcanisa . 3 C. [REEP basalt deposits in the Imbrium Region. -
Regolith Compaction and Its Implications for the Formation Mechanism of Lunar Swirls
EPSC Abstracts Vol. 13, EPSC-DPS2019-1608-1, 2019 EPSC-DPS Joint Meeting 2019 c Author(s) 2019. CC Attribution 4.0 license. Regolith Compaction and its Implications for the Formation Mechanism of Lunar Swirls Christian Wöhler (1), Megha Bhatt (2), Arne Grumpe (1), Marcel Hess (1), Alexey A. Berezhnoy (3), Vladislav V. Shevchenko (3) and Anil Bhardwaj (2) (1) Image Analysis Group, TU Dortmund University, Otto-Hahn-Str. 4, 44227 Dortmund, Germany, (2) Physical Research Laboratory, Ahmedabad, 380009, India, (3) Sternberg Astronomical Institute, Universitetskij pr., 13, Moscow State University, 119234 Moscow, Russia ([email protected]) Abstract The brightening of the regolith at Reiner Gamma could be a result of reduced space-weathering due to In this study we have examined spectral trends of magnetic shielding [3] and/or due to soil compaction Reiner Gamma (7.5°N, 59°W) using the Moon [5]. According to the model of [9], the spectral Mineralogy Mapper (M3) [1] observations. We variation due to soil compaction is a change in albedo derived maps of solar wind induced OH/H2O and a with negligible effect on spectral slope and compaction index map of the Reiner Gamma swirl. absorption band depths. To quantify soil compaction Our results suggest that the combination of soil at Reiner Gamma, we empirically defined the compaction and magnetic shielding can explain the compaction index c as a positive real number given observed spectral trends. These new findings support by c = M / RSE, where M is the reflectance the hypothesis of swirl formation by interaction modulation at 1.579 µm between a bright on-swirl between a comet and the uppermost regolith layer. -
Tracing Subduction Zone Processes with Magnesium Isotopes
Tracing subduction zone processes with magnesium isotopes Yan Hu A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy University of Washington 2018 Reading Committee: Fang-Zhen Teng, Chair Bruce K. Nelson Ronald S. Sletten Program Authorized to Offer Degree: Earth and Space Sciences © Copyright 2018 Yan Hu University of Washington Abstract Tracing subduction zone processes with magnesium isotopes Yan Hu Chair of the Supervisory Committee: Professor Fang-Zhen Teng Department of Earth and Space Sciences Subduction and recycling of oceanic plates change the chemical composition of mantle and affect its physical properties, thereby modulating Earth’s dynamics. Stable Mg isotopes (δ26Mg) can trace this recycling process as crustal materials are highly fractionated compared to the average mantle composition. This dissertation focuses on Mg isotope fractionation during subduction-related processes and the consequent mantle heterogeneity. The dissertation first compares inconsistent δ26Mg values of San Carlos peridotitic olivines that are published by several laboratories. We analyzed mineral grains from two San Carlos peridotites with disparate lithologies and determined that all mineral phases have indistinguishable δ26Mg values to within 0.07‰. With analytical precision and accuracy being confirmed, the significance of anomalous δ26Mg values can be understood in the context of mantle heterogeneity. The next paper investigates the Mg isotopic heterogeneity in mantle pyroxenites that have formed by multi-stage interactions between peridotites and melts with diverse origins. Pyroxenites formed by reaction with melts derived from subducted oceanic crust and carbonate sediments are shown to have variable δ26Mg values (−1.51‰ to −0.10‰). In contrast, pyroxenites that are formed by reaction with silicate melts from deep mantle has δ26Mg values similar to common mantle peridotites. -
Science Concept 5: Lunar Volcanism Provides a Window Into the Thermal and Compositional Evolution of the Moon
Science Concept 5: Lunar Volcanism Provides a Window into the Thermal and Compositional Evolution of the Moon Science Concept 5: Lunar volcanism provides a window into the thermal and compositional evolution of the Moon Science Goals: a. Determine the origin and variability of lunar basalts. b. Determine the age of the youngest and oldest mare basalts. c. Determine the compositional range and extent of lunar pyroclastic deposits. d. Determine the flux of lunar volcanism and its evolution through space and time. INTRODUCTION Features of Lunar Volcanism The most prominent volcanic features on the lunar surface are the low albedo mare regions, which cover approximately 17% of the lunar surface (Fig. 5.1). Mare regions are generally considered to be made up of flood basalts, which are the product of highly voluminous basaltic volcanism. On the Moon, such flood basalts typically fill topographically-low impact basins up to 2000 m below the global mean elevation (Wilhelms, 1987). The mare regions are asymmetrically distributed on the lunar surface and cover about 33% of the nearside and only ~3% of the far-side (Wilhelms, 1987). Other volcanic surface features include pyroclastic deposits, domes, and rilles. These features occur on a much smaller scale than the mare flood basalts, but are no less important in understanding lunar volcanism and the internal evolution of the Moon. Table 5.1 outlines different types of volcanic features and their interpreted formational processes. TABLE 5.1 Lunar Volcanic Features Volcanic Feature Interpreted Process -
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, -
Intrusives and Lava Tubes: Potential Lunar Swirl Source Bodies? S
49th Lunar and Planetary Science Conference 2018 (LPI Contrib. No. 2083) 2587.pdf INTRUSIVES AND LAVA TUBES: POTENTIAL LUNAR SWIRL SOURCE BODIES? S. M. Tikoo1 and D. J. Hemingway2, 1Department of Earth and Planetary Sciences, Rutgers University, Piscataway Township, NJ ([email protected]), 2Department of Earth and Planetary Science, University of California, Berkeley, CA. Introduction: Lunar swirls are enigmatic albedo ferromagnetic grains or create new ones. This process features that appear in several regions across the lunar is exemplified by heating experiments on lunar sam- surface (e.g., ref. [1]) and consist of bright and dark ples or their analogs in a controlled oxygen fugacity markings alternating over length scales of typically 1– environment. Heating synthetic mare basalts in a re- 5 km. Most swirls are not readily associated with con- ducing atmosphere ~1 log unit below the iron-wustite spicuous geological features, such as impact craters buffer (i.e., IW-1; the oxygen fugacity conditions in- (e.g., the archetypal swirl at Reiner Gamma lies atop a ferred for a majority of lunar rocks studied thus far) to relatively smooth mare plain) but instead appear to be temperatures in excess of 600°C has produced subsoli- surficial in nature. Swirls are most plausibly the result dus reduction of ilmenite and the associated growth of metal (Fig. 1) [6]. of electrostatically or magnetically-driven sorting of regolith fines [2,3] or solar wind interactions with lo- calized remanent crustal magnetism (e.g., ref. [4]). In either scenario, the complex geometry of the albedo pattern must be a function of the structure of the near surface magnetic field. -
Landed Science at a Lunar Crustal Magnetic Anomaly
Landed Science at a Lunar Crustal Magnetic Anomaly David T. Blewett, Dana M. Hurley, Brett W. Denevi, Joshua T.S. Cahill, Rachel L. Klima, Jeffrey B. Plescia, Christopher P. Paranicas, Benjamin T. Greenhagen, Lauren Jozwiak, Brian A. Anderson, Haje Korth, George C. Ho, Jorge I. Núñez, Michael I. Zimmerman, Pontus C. Brandt, Sabine Stanley, Joseph H. Westlake, Antonio Diaz-Calderon, R. Ter ik Daly, and Jeffrey R. Johnson Space Science Branch, Johns Hopkins University Applied Physics Lab, USA Lunar Science for Landed Missions Workshop – January, 2018 1 Lunar Magnetic Anomalies • The lunar crust contains magnetized areas, a few tens to several hundred kilometers across, known as "magnetic anomalies". • The crustal fields are appreciable: Strongest anomalies are ~10-20 nT at 30 km altitude, perhaps a few hundred to 1000 nT at the surface. Lunar Prospector magnetometer Btot map (Richmond & Hood 2008 JGR) over LROC WAC 689-nm mosaic 2 Lunar Magnetic Anomalies: Formation Hypotheses • Magnetized basin ejecta: ambient fields amplified by compression as impact-generated plasma converged on the basin antipode (Hood and co-workers) Lunar Prospector magnetometer Btot (Richmond & Hood 2008 JGR) over LROC WAC 689- nm mosaic 3 Lunar Magnetic Anomalies: Formation Hypotheses • Magnetized basin ejecta: ambient fields amplified by compression as impact-generated plasma converged on the basin antipode (Hood and co-workers) • Magnetic field impressed on the surface by plasma interactions when a cometary coma struck the Moon (Schultz) Lunar Prospector magnetometer Btot (Richmond & Hood 2008 JGR) over LROC WAC 689- nm mosaic 4 Lunar Magnetic Anomalies: Formation Hypotheses • Magnetized basin ejecta: ambient fields amplified by compression as impact-generated plasma converged on the basin antipode (Hood and co-workers) • Magnetic field impressed on the surface by plasma interactions when a cometary coma struck the Moon (Schultz) • Magmatic intrusion or impact melt magnetized in an early lunar dynamo field (e.g., Purucker et al. -
The Choice of the Location of the Lunar Base N93-17431
155 PRECEDING PhGE ,,=,_,,c,;_''_'" t¢OT F|Lf_D THE CHOICE OF THE LOCATION OF THE LUNAR BASE N93-17431 V. V. Y__hevchenko P.. K _ AsO_nomtca/In./lute Moscow U_ Moscow 119899 USSR The development of modern methods of remote sensing of the lunar suuface and data from lunar studies by space vehicles make it possgale to assess scientifically the e:qOediowy of the locationof the lunar base in a definite region on the Moon. The prefimlnary choice of the site is important for tackling a range of problems assocfated with ensuring the activity of a manned lunar base and with fulfilh'ng the research program. Based on astronomical dat_ we suggest the Moon's western _, specifically the western part of Oceanus Proceliarurtg where natural scientifically interesting objects have been identifle_ as have surface rocks with enlaanced contents of ilmenite, a poss_le source of oxygen. A comprehensive et_tluation of the region shows timt, as far as natural features are concernetg it is a key one for solving the main problems of the Moon's orlgln and evolution. INTRODUCTION final period of shaping the lunar crust's upper horizons (this period coincided with the final equalization of the Moon's periods The main criteria for choosing a site for the first section of a of orbital revolution and axial rotation), the impact of terrestrial manned lunar base are (1)the most favorable conditions for gravitation on the internal structure of the Moon increased. transport operations, (2)the presence of natural objects of Between 4 and 3 b.y. -
An Examination of Mare Age Based On
An Examination of Mare Age Based On Cratering Density The Chenango Forks Lunar Research Team: Sharon Hartzell, Jackson Haskell, Benjamin Daniels, Sarah Maximowicz, and Sarah Andrus Objective Cooled basaltic lava flows, known as maria, cover approximately sixteen percent of the lunar surface. The determination of absolute and relative ages of maria is an important question in lunar research, because it provides insight into the geologic history of the lunar environment. Many samples returned from the Apollo and Luna missions have been absolutely dated using radiogenic techniques. However, not all samples returned from the moon have been radiogenically dated. Furthermore, returned samples represent only a small portion of each visited mare. One of the major challenges facing lunar researches is the fact that most maria are still unvisited. The lack of complete data from visited maria in combination with the absence of data from unvisited maria has compelled lunar researchers to rely on remote techniques for relative dating. The overriding goal of our research was to develop and utilize a method for analyzing the ages of the twenty‐three lunar maria. Approach •Areas of the twenty‐three lunar maria were analyzed in three distinct investigations. Investigation 1: Total crater count to determine cratering densities, and comparison of densities to absolute age Investigation 2: Analysis of crater weathering in relation to age Investigation 3: Analysis of crater size in relation to age •A relative age map was created to display the distribution of the maria on the moon’s surface. The •Analysis of age dist ributions within individual mari a revealed several interesting trends: Investigation 1 map itself was obtained from Google Moon, and the maria were highlighted based on the scale Method displayed below. -
Applications of Solar Wind Particle Impact Simulations at Lunar Magnetic Anomalies to the Study of Lunar Swirls
47th Lunar and Planetary Science Conference (2016) 2648.pdf APPLICATIONS OF SOLAR WIND PARTICLE IMPACT SIMULATIONS AT LUNAR MAGNETIC ANOMALIES TO THE STUDY OF LUNAR SWIRLS. C. J. Tai Udovicic1, G. Y. Kramer2, and E. M. Harnett3, 1Dept of Earth Sciences, University of Toronto, 22 Russell St, Toronto, ON, Canada, ([email protected]), 2Lunar and Planetary Institute, 3600 Bay Area Bvld, Houston, TX, ([email protected]), 3University of Washington, Earth and Space Sciences, Seattle, WA ([email protected]). Introduction: Lunar swirls are high albedo features highlands often appear to have swirl-like anomalies due that exhibit low spectral maturity. They have been to their complicated topography. To mitigate this, we identified at various sites on the Moon, and all coincide generated a slope map from the WAC GLD100 (SLP), with a lunar magnetic anomaly (magnomaly) [1], which we overlayed with the WAC 643 nm normalized although not all magnomalies have an identifiable swirl. reflectance image to distinguish high albedo swirls from The leading hypothesis for lunar swirl origin is high albedo slopes. Even so, after one pass of the region, presented in [2] as magnetic field standoff of the solar only about half of the swirls could be detected with this wind which causes uneven space weathering at the swirl method alone. The remaining half were found after surface. This hypothesis fails to explain why lunar using particle simulations as a guide. swirls are observed at some but not all of the magnetic Solar wind particle tracking simulations: We anomalies present on the Moon. To investigate the solar used the 2D solar wind particle tracking simulation wind standoff hypothesis further and to improve swirl presented in [2]. -
Patent Infringement in Outer Space in Light of 35 U.S.C. § 105
THIS VERSION DOES NOT CONTAIN PARAGRAPH/PAGE REFERENCES. PLEASE CONSULT THE PRINT OR ONLINE DATABASE VERSIONS FOR PROPER CITATION INFORMATION. ARTICLE PATENT INFRINGEMENT IN OUTER SPACE IN LIGHT OF 35 U.S.C. § 105: FOLLOWING THE WHITE RABBIT DOWN THE RABBIT LOOPHOLE THEODORE U. RO* MATTHEW J. KLEIMAN** KURT G. HAMMERLE*** * Theodore (Ted) Ro is an intellectual property attorney at Johnson Space Center, working for the National Aeronautics and Space Administration. Mr. Ro has a Bachelor of Science degree in aerospace engineering from Texas A&M University as well as a master’s degree in industrial engineering and a Doctor of Jurisprudence from the University of Houston. Mr. Ro primarily practices in the area of intellectual property law, including patent prosecu- tion and patent licensing. ** Matthew Kleiman is Corporate Counsel at the Draper Laboratory in Cambridge, MA. Mr. Kleiman also chairs the Space Law Committee of the ABA Section on Science & Tech- nology Law and teaches Space Law at Boston University School of Law. Mr. Kleiman earned his Bachelor of Arts degree from Rutgers University and Doctor of Jurisprudence from Duke University. *** Kurt G. Hammerle is an intellectual property attorney for the National Aeronautics and Space Administration at the Lyndon B. Johnson Space Center located in Houston, TX. Mr. Hammerle earned a Bachelor of Science degree in mechanical engineering from Virginia Polytechnic Institute & State University in 1988 and a Doctor of Jurisprudence from the Marshall-Wythe School of Law at the College of William & Mary in 1991. The views expressed herein are those of the authors’ and not of the National Aeronautics and Space Administration, Draper Laboratory or any other organization.