Geology of 243 Ida
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Potential Resources on and from the Asteroids/Comets; Threats
ASTEROIDS AND COMETS: POTENTIAL RESOURCES LECTURE 21 NEEP 533 HARRISON H. SCHMITT EROS C-TYPE NASA/NEAR SHOEMAKER/APL 11X11X34 KM ASTEROIDS IN GENERAL 1.3 GM/CM3 MAIN BELT ASTEROIDS BETWEEN JUPITER AND MARS NEAR EARTH ASTEROIDS SOME MAY BE SPENT COMETS EARTH CROSSING ASTEROIDS SOME MAY BE SPENT COMETS “CENTAUR” ASTEROIDS BETWEEN JUPITER AND URANUS CHIRON, 1979 VA, AND 133P/ELST-PIZARRO ALSO HAVE COMET- LIKE BEHAVIOR “TROJAN” ASTEROIDS JUPITER’S ORBIT AND CONTROLLED BY IT GENERAL CHARACTERISTICS RUBBLE PILES (?) NO ASTEROID >150M ROTATES FASTER THAN ONE REVOLUTION PER 2 HOURS CALCULATED LIMIT FOR RUBBLE TO STAY TOGETHER 1998 KY26 IS 30M IN DIAMETER, ROTATES IN 10.7 MIN. AND MAY BE SOLID MAY BE A TRANSITION IN ORBITAL CHARACTERISTICS AND / OR COMPOSITION BETWEEN SOME ASTEROIDS AND COMETS • S-TYPE OTHER ASTEROIDS – INNER ASTEROID BELT – EVIDENCE OF HEATING AND DIFFERENTIATION – 29 TELESCOPIC SPECTRA (Binzel, et al., 1996) • INTERMEDIATE BETWEEN S-TYPE AND ORDINARY CHONDRITES – 1. DISTINCT ROCK TYPES VS DIVERSE LARGER BODIES – 2. ABUNDANCE OF OPAQUE MATERIALS – 3. FRESH SURFACES (MOST LIKELY) • BASALTIC ACHONDRITES (6%) – 4 VESTA AT 2.36 AU [MAIN BELT PARENT (?)] – TOUTATIS - NEA (RADAR STUDY) • 4.5X2.4X1.9KM, 2.1 GM/CM3, TWO ROTATIONS, I.E., TUMBLING (5.4 AND 7.3 DAYS) – 1459 MAGNYA AT 3.15 AU [FRAGMENT OF LARGER BODY (?)] EROS • (Lazzaro, et al, 2000, Science, 288) C-TYPE (REVISED BY GRS DATA) 11X11X33 KM 2.7 GM/CM3 5.27 HR ROTATION NASA/NEAR SHOEMAKER/APL OTHER ASTEROIDS • D-TYPE CARBONACEOUS CHONDRITE (BEYOND MAIN BELT ASTEROIDS) – TAGISH -
Asteroid Strike! Near-Earth Asteroids
Asteroid Attack! Asteroid Attack! asteroid 243 Ida A few years ago, astronomers discovered a mile-wide rock tumbling through space. At first, the scientists feared that the newly discovered space rock would plow into Earth on February 1, 2019. Scientists named the space rock NT7 and clocked its speed at 7 miles per second. The scientists thought the asteroid was heading straight for Earth! Asteroid Strike! A mile-wide asteroid could take out an entire continent, scientists say. Fearing the worst, scientists kept their eyes on NT7. They plotted its orbit, or path, around the sun. After watching NT7 for several weeks, scientists found out that NT7 would miss Earth on February 1, 2019. Near-Earth Asteroids ReadWorks.org Copyright © 2009 Weekly Reader Corporation. All rights reserved. Used by permission.Weekly Reader is a registered trademark of Weekly Reader Corporation. Asteroid Attack! Most asteroids orbit the sun between Mars and Jupiter. NT7, however, is a near-Earth asteroid. Near-Earth asteroids orbit the sun close to Earth. NT7 orbits the sun once every 837 days. Its orbit sometimes takes NT7 as far from the sun as Mars. At other times, it is within Earth's orbit. Scientists know about nearly 350 near-Earth asteroids. They carefully map the orbits of those asteroids to make sure the asteroids don't come too close to our planet. Scientists say anywhere from 500 to 1,000 near-Earth asteroids are yet to be discovered. Scientists are searching the sky for them. They want to have plenty of warning if one comes too close. -
Precision Astrometry for Fundamental Physics – Gaia
Gravitation astrometric tests in the external Solar System: the QVADIS collaboration goals M. Gai, A. Vecchiato Istituto Nazionale di Astrofisica [INAF] Osservatorio Astrofisico di Torino [OATo] WAG 2015 M. Gai - INAF-OATo - QVADIS 1 High precision astrometry as a tool for Fundamental Physics Micro-arcsec astrometry: Current precision goals of astrometric infrastructures: a few 10 µas, down to a few µas 1 arcsec (1) 5 µrad 1 micro-arcsec (1 µas) 5 prad Reference cases: • Gaia – space – visible range • VLTI – ground – near infrared range • VLBI – ground – radio range WAG 2015 M. Gai - INAF-OATo - QVADIS 2 ESA mission – launched Dec. 19th, 2013 Expected precision on individual bright stars: 1030 µas WAG 2015 M. Gai - INAF-OATo - QVADIS 3 Spacetime curvature around massive objects 1.5 G: Newton’s 1".74 at Solar limb 8.4 rad gravitational constant GM 1 cos d: distance Sun- 1 1 observer c2d 1 cos M: solar mass 0.5 c: speed of light Deflection [arcsec] angle : angular distance of the source to the Sun 0 0 1 2 3 4 5 6 Distance from Sun centre [degs] Light deflection Apparent variation of star position, related to the gravitational field of the Sun ASTROMETRY WAG 2015 M. Gai - INAF-OATo - QVADIS 4 Precision astrometry for Fundamental Physics – Gaia WAG 2015 M. Gai - INAF-OATo - QVADIS 5 Precision astrometry for Fundamental Physics – AGP Talk A = Apparent star position measurement AGP: G = Testing gravitation in the solar system Astrometric 1) Light deflection close to the Sun Gravitation 2) High precision dynamics in Solar System Probe P = Medium size space mission - ESA M4 (2014) Design driver: light bending around the Sun @ μas fraction WAG 2015 M. -
A Survey of the Planets Mercury Difficult to Observe
A Survey of the Planets Earth [Slides] N ,O ,H 0 atmosphere Mercury 2 2 2 Difficult to observe - never more than Surface area 71% H20 28 degree angle from the Sun. Prograde rotation 23hr 56min 04.1sec Mariner 10 flyby (1974) =>Why do we use a 24 hour clock? Found cratered terrain. Weathered, tectonic, volcanic, Messenger Orbiter (Launch 2004; Orbit 2009) and cratered surface. Rotation is 59 days (discovered by MIT) Thin sodium (Na) atmosphere - recent discovery One satellite (large relative to its primary). No Moons. Moon Venus Cratered surface - formed by impacts A near twin to Earth in size and mass Mare - (“seas”) formed by lava flows Dense CO atmosphere 2 Regolith - soil Surface pressure ~90 bars (earth atm = 1 bar) Age: 4.5 Gy - same as rest of solar system Surface temperature ~750 K (0 K = -273 C) 9 Retrograde rotation, 243 days (Gy = 10 years) 0 - 0.5 Gy -heavy bombardment (Prograde rotation is West -> East) (Retrograde rotation is East ->West) 1.0 - 2.5 Gy - lava flows forming Mare Surface volcanic features, vast resurfacing 2.5-4.5 Gy - less frequent bombardment of entire planet about 1 billion years ago. Origin of the Moon? No Moons. Mariner, Pioneer, Venera: Flybys, orbiters, landers (1960s, 1970s) Magellan Mission 1989 - Radar mapping to 100m resolution (headed by MIT). 1 2 Mars Asteroids First one (Ceres) discovered in 1801 Thin CO2 atmosphere Surface Pressure ~6 mbar (0.6% of Earth) Location (2.8 AU) fit Bode!s Rule There are >10,000 known asteroids Surface Temperature: 190 to 240 K (-83 C to -33 C) Most orbit between Mars and Jupiter, region called the “asteroid belt” Rotation is 24.5 hours, prograde Sizes range from boulders - 1000 km A Disrupted planet? <----No Cratered surface, volcanoes, chasms Probably left-over planetesimals from Evidence for water flow! (Where is it now?) formation of the solar system. -
A Visit to Gaspra
A Visit to Gaspra This is a ground-based photo of the first minor planet ever to be visited by a spacecraft. On October 29, 1991, the NASA spacecraft Galileo flew past minor planet No. 951 Gaspra on its way to Jupiter where it will arrive in De- cember 1995. The distance to Gaspra from the Earth was 410 million km at the time of the fly-by. Although Galilw's high-galn antenna has not yet been un- folded and could therefore not be used, JPL engineers succeeded In getting a 300-line Image via the low-gain antenna; the others will be sent when Gallleo is again near the Earth. The first image showed the irregular form of Gaspra and Several craters on its surface with a res- otution of ht130 metres. The diarne- ter was measured as 16 kilornetms. Gaspra was discovered on July 30, 191 6 at the Simeis Observatq in the mountains of Cximea, the Russia. The sofi on the southern coast of Crimea, in On this date, Its distance from the Earth discoverer was the welt-known Russian which the famous Russian writer Lev was 262 million km and the magnitude astronomer Grigorij Nikolaevich Neuj- Nikolaevfch Tolstoy (1828- 1910) spent was about 15. min (born 1886 in Tbilisi, Georgia; died many years of his life." The village of The background of the photo is a I946 in Leningrad), who later became Gaspra is located about 10 krn south- region in the southern constellation Director of that observatory (1925- 1931 west of Yalta. Ophlochus (the Serpent-holder) which is and 1936-1941) and Director of the The present photo was obtained with characterld by relatively few stars, but Pulkovo Obsewatoty near St. -
Phase Integral of Asteroids Vasilij G
A&A 626, A87 (2019) Astronomy https://doi.org/10.1051/0004-6361/201935588 & © ESO 2019 Astrophysics Phase integral of asteroids Vasilij G. Shevchenko1,2, Irina N. Belskaya2, Olga I. Mikhalchenko1,2, Karri Muinonen3,4, Antti Penttilä3, Maria Gritsevich3,5, Yuriy G. Shkuratov2, Ivan G. Slyusarev1,2, and Gorden Videen6 1 Department of Astronomy and Space Informatics, V.N. Karazin Kharkiv National University, 4 Svobody Sq., Kharkiv 61022, Ukraine e-mail: [email protected] 2 Institute of Astronomy, V.N. Karazin Kharkiv National University, 4 Svobody Sq., Kharkiv 61022, Ukraine 3 Department of Physics, University of Helsinki, Gustaf Hällströmin katu 2, 00560 Helsinki, Finland 4 Finnish Geospatial Research Institute FGI, Geodeetinrinne 2, 02430 Masala, Finland 5 Institute of Physics and Technology, Ural Federal University, Mira str. 19, 620002 Ekaterinburg, Russia 6 Space Science Institute, 4750 Walnut St. Suite 205, Boulder CO 80301, USA Received 31 March 2019 / Accepted 20 May 2019 ABSTRACT The values of the phase integral q were determined for asteroids using a numerical integration of the brightness phase functions over a wide phase-angle range and the relations between q and the G parameter of the HG function and q and the G1, G2 parameters of the HG1G2 function. The phase-integral values for asteroids of different geometric albedo range from 0.34 to 0.54 with an average value of 0.44. These values can be used for the determination of the Bond albedo of asteroids. Estimates for the phase-integral values using the G1 and G2 parameters are in very good agreement with the available observational data. -
Iso and Asteroids
r bulletin 108 Figure 1. Asteroid Ida and its moon Dactyl in enhanced colour. This colour picture is made from images taken by the Galileo spacecraft just before its closest approach to asteroid 243 Ida on 28 August 1993. The moon Dactyl is visible to the right of the asteroid. The colour is ‘enhanced’ in the sense that the CCD camera is sensitive to near-infrared wavelengths of light beyond human vision; a ‘natural’ colour picture of this asteroid would appear mostly grey. Shadings in the image indicate changes in illumination angle on the many steep slopes of this irregular body, as well as subtle colour variations due to differences in the physical state and composition of the soil (regolith). There are brighter areas, appearing bluish in the picture, around craters on the upper left end of Ida, around the small bright crater near the centre of the asteroid, and near the upper right-hand edge (the limb). This is a combination of more reflected blue light and greater absorption of near-infrared light, suggesting a difference Figure 2. This image mosaic of asteroid 253 Mathilde is in the abundance or constructed from four images acquired by the NEAR spacecraft composition of iron-bearing on 27 June 1997. The part of the asteroid shown is about 59 km minerals in these areas. Ida’s by 47 km. Details as small as 380 m can be discerned. The moon also has a deeper near- surface exhibits many large craters, including the deeply infrared absorption and a shadowed one at the centre, which is estimated to be more than different colour in the violet than any 10 km deep. -
(2000) Forging Asteroid-Meteorite Relationships Through Reflectance
Forging Asteroid-Meteorite Relationships through Reflectance Spectroscopy by Thomas H. Burbine Jr. B.S. Physics Rensselaer Polytechnic Institute, 1988 M.S. Geology and Planetary Science University of Pittsburgh, 1991 SUBMITTED TO THE DEPARTMENT OF EARTH, ATMOSPHERIC, AND PLANETARY SCIENCES IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY IN PLANETARY SCIENCES AT THE MASSACHUSETTS INSTITUTE OF TECHNOLOGY FEBRUARY 2000 © 2000 Massachusetts Institute of Technology. All rights reserved. Signature of Author: Department of Earth, Atmospheric, and Planetary Sciences December 30, 1999 Certified by: Richard P. Binzel Professor of Earth, Atmospheric, and Planetary Sciences Thesis Supervisor Accepted by: Ronald G. Prinn MASSACHUSES INSTMUTE Professor of Earth, Atmospheric, and Planetary Sciences Department Head JA N 0 1 2000 ARCHIVES LIBRARIES I 3 Forging Asteroid-Meteorite Relationships through Reflectance Spectroscopy by Thomas H. Burbine Jr. Submitted to the Department of Earth, Atmospheric, and Planetary Sciences on December 30, 1999 in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy in Planetary Sciences ABSTRACT Near-infrared spectra (-0.90 to ~1.65 microns) were obtained for 196 main-belt and near-Earth asteroids to determine plausible meteorite parent bodies. These spectra, when coupled with previously obtained visible data, allow for a better determination of asteroid mineralogies. Over half of the observed objects have estimated diameters less than 20 k-m. Many important results were obtained concerning the compositional structure of the asteroid belt. A number of small objects near asteroid 4 Vesta were found to have near-infrared spectra similar to the eucrite and howardite meteorites, which are believed to be derived from Vesta. -
Magnetic Field Measurements During the ROSETTA Flyby at Asteroid
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Institute of Transport Research:Publications Planetary and Space Science ] (]]]]) ]]]–]]] Contents lists available at SciVerse ScienceDirect Planetary and Space Science journal homepage: www.elsevier.com/locate/pss Magnetic field measurements during the ROSETTA flyby at asteroid (21)Lutetia I. Richter a,n, H.U. Auster a, K.H. Glassmeier a,b, C. Koenders a,b, C.M. Carr c, U. Motschmann d,e, J. Muller¨ d, S. McKenna-Lawlor f a Institut fur¨ Geophysik und extraterrestrische Physik, Technische Universitat¨ Braunschweig, Mendelssohnstr. 3, 38106 Braunschweig, Germany b Max Planck Institute for Solar System Research, Lindau, Germany c Imperial College London, London, UK d Institut fur¨ theoretische Physik, Technische Universitat¨ Braunschweig, Mendelssohnstr. 3, 38106 Braunschweig, Germany e DLR-Institut fur¨ Planetenforschung, Rutherfordstr. 2, 12489 Berlin, Germany f Space Technology Ireland, National University of Ireland Maynooth, Co. Kildare, Ireland article info abstract Article history: On July 10, 2010, the ROSETTA spacecraft performed a flyby at asteroid (21)Lutetia at a solar distance of Received 13 May 2011 2.72 AU. The spacecraft–asteroid distance at closest approach was 3120 km. The magnetometers Received in revised form onboard ROSETTA were operating but did not detect any conclusive signature of the asteroid. 18 August 2011 Any magnetic field signature which could possibly be attributed to the asteroid was below 1 nT. Accepted 19 August 2011 Consequently an upper limit for the global magnetic properties of asteroid (21)Lutetia could be derived: À maximum dipole moment r1:0 Â 1012 Am2, global maximum magnetization r2:1 Â 10 3 A=m, À Keywords: specific moment r5:9 Â 10 7 Am2=kg. -
Binary Asteroid Lightcurves
BINARY ASTEROID LIGHTCURVES Asteroid Type Per1 Amp1 Per2 Amp2 Perorb Ds/Dp a/Dp Reference 22 Kalliope B 4.1483 0.53 B a Descamps, 08 B a 86.2896 Marchis, 08 B a 4.148 86.16 Marchis, 11w 41∗ Daphne B 5.988 0.45 B s 26.4 Conrad, 08 B s 38. Conrad, 08 B s 5.987981 27.289 2.46 Carry, 18 45 Eugenia M 5.699 0.30 B a 113. Merline, 99 B a Marchis, 06 M a Marchis, 07 M a Marchis, 08 B a 5.6991 114.38 Marchis, 11w 87 Sylvia M 5.184 0.50 M a 5.184 87.5904 Marchis, 05 M a 5.1836 87.59 Marchis, 11w 90∗ Antiope B 16.509 0.88 B f 16. Merline, 00 B f 16.509 0.73 16.509 0.73 16.509 Descamps, 05 B f 16.5045 0.86 16.5045 0.86 16.5045 Behrend, 07w B f 16.505046 16.505046 Bartczak, 14 93 Minerva M 5.982 0.20 M a 5.982 0.20 57.79 Marchis, 11 107∗ Camilla M 4.844 0.53 B a Marchis, 08 B a 4.8439 89.04 Marchis, 11w M a 1.550 Marsset, 16 M s 89.096 4.91 Pajuelo, 18 113 Amalthea B? 9.950 0.22 ? u Maley, 17 121 Hermione B 5.55128 0.62 B a Merline, 02 B a Marchis, 04 B a Marchis, 05 B a 5.55 61.97 Marchis, 11w 130 Elektra M 5.225 0.58 B a 5.22 126.2 Marchis, 08 M a Yang, 14 216 Kleopatra M 5.385 1.22 M a 5.38 Marchis, 08 243 Ida B 4.634 0.86 B a Belton, 94 279 Thule B? 23.896 0.10 B s 7.44 0.08 72.2 Sato, 15 283 Emma B 6.896 0.53 B a Merline, 03 B a 6.89 80.48 Marchis, 08 324 Bamberga B? 29.43 0.12 B s 29.458 0.06 71.0 Sato, 15 379 Huenna B 14.141 0.12 B a Margot, 03 B a 4.022 2102. -
Debris About Asteroids: Where and How Much?
Asteroids, Comets, Meteors 1991, pp. 101-108 Lunar and Planetarylnstitute, Houston, 1992 _ // /-7/0 _7"_ 10l DEBRIS ABOUT ASTEROIDS: WHERE AND HOW MUCH? - Joseph A. Burns and Douglas P. Hamilton Cornell University, Ithaca NY 14853 USA i We summarize several recent findings on the size and shape of the region within which material can ! i ! stably orbit an asteroid. If the asteroid (with assumed density 2.38 g/cm 3) circles the Sun at 2.55 AU, | co-planar prograde material will remain trapped whenever started on unperturbed circular orbits at ! less than about 220 R A (asteroid radii); co-planar retrograde particles are stable out twice as far. Our 3-D stability surface, which encloses several hundred numerically calculated orbits that start with various inclinations, is shaped like a sphere with its top and bottom sliced off; its dimensions scale like the Hill radius =(p./3)1/3R, where p. is the asteroid-to-solar mass ratio and R is the asteroid's orbital radius. If the asteroid moves along an elliptical orbit, a fairly reliable indicator of the dimensions of the hazard zone is the size of its Hill sphere at the orbit's pericenter. Grains with radii less than a few mm will be lost through the action of radiation forces which can induce escape or cause collisions with the asteroid on time scales of a few years; interplanetary micrometeoroids produce collisional break-up of these particles in ~104 yrs. The effects of Jupiter and of asteroids that pass close to the target asteroid allow particles to diffuse from the system, again shrinking the hazard zone. -
Dust Phenomena Relating to Airless Bodies
Space Sci Rev (2018) 214:98 https://doi.org/10.1007/s11214-018-0527-0 Dust Phenomena Relating to Airless Bodies J.R. Szalay1 · A.R. Poppe2 · J. Agarwal3 · D. Britt4 · I. Belskaya5 · M. Horányi6 · T. Nakamura7 · M. Sachse8 · F. Spahn 8 Received: 8 August 2017 / Accepted: 10 July 2018 © Springer Nature B.V. 2018 Abstract Airless bodies are directly exposed to ambient plasma and meteoroid fluxes, mak- ing them characteristically different from bodies whose dense atmospheres protect their surfaces from such fluxes. Direct exposure to plasma and meteoroids has important con- sequences for the formation and evolution of planetary surfaces, including altering chemical makeup and optical properties, generating neutral gas and/or dust exospheres, and leading to the generation of circumplanetary and interplanetary dust grain populations. In the past two decades, there have been many advancements in our understanding of airless bodies and their interaction with various dust populations. In this paper, we describe relevant dust phenomena on the surface and in the vicinity of airless bodies over a broad range of scale sizes from ∼ 10−3 km to ∼ 103 km, with a focus on recent developments in this field. Keywords Dust · Airless bodies · Interplanetary dust Cosmic Dust from the Laboratory to the Stars Edited by Rafael Rodrigo, Jürgen Blum, Hsiang-Wen Hsu, Detlef Koschny, Anny-Chantal Levasseur-Regourd, Jesús Martín-Pintado, Veerle Sterken and Andrew Westphal B J.R. Szalay [email protected] A.R. Poppe [email protected] 1 Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08540, USA 2 Space Sciences Laboratory, U.C. Berkeley, Berkeley, CA, USA 3 Max Planck Institute for Solar System Research, Göttingen, Germany 4 University of Central Florida, Orlando, FL 32816, USA 5 Institute of Astronomy, V.N.