Limb Profiles of the Moon from Grazing Occultation Observations
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Advances in the Interpretation and Analysis of Lunar Occultation Light Curves
A&A 538, A56 (2012) Astronomy DOI: 10.1051/0004-6361/201118476 & c ESO 2012 Astrophysics Advances in the interpretation and analysis of lunar occultation light curves A. Richichi1,2 and A. Glindemann2 1 National Astronomical Research Institute of Thailand, 191 Siriphanich Bldg., Huay Kaew Rd., Suthep, Muang, Chiang Mai 50200, Thailand e-mail: [email protected] 2 European Southern Observatory, Karl-Schwarzschild-Str. 2, 85748 Garching bei München, Germany Received 18 November 2011 / Accepted 23 December 2011 ABSTRACT Context. The introduction of fast 2D detectors and the use of very large telescopes have significantly advanced the sensitivity and accuracy of the lunar occultation technique. Recent routine observations at the ESO Very Large Telescope have yielded hundreds of events with results, especially in the area of binary stars, which are often beyond the capabilities of any other techniques. Aims. With the increase in the quality and in the number of the events, subtle features in the light curve patterns have occasionally been detected which challenge the standard analytical definition of the lunar occultation phenomenon as diffraction from an infinite straight edge. We investigate the possible causes for the observed peculiarities. Methods. We have evaluated the available statistics of distortions in occultation light curves observed at the ESO VLT, and compared it to data from other facilities. We have developed an alternative approach to model and interpret lunar occultation light curves, based on 2D diffraction integrals describing the light curves in the presence of an arbitrary lunar limb profile. We distinguish between large limb irregularities requiring the Fresnel diffraction formalism, and small irregularities described by Fraunhofer diffraction. -
The Surrender Software
Scientific image rendering for space scenes with the SurRender software Scientific image rendering for space scenes with the SurRender software R. Brochard, J. Lebreton*, C. Robin, K. Kanani, G. Jonniaux, A. Masson, N. Despré, A. Berjaoui Airbus Defence and Space, 31 rue des Cosmonautes, 31402 Toulouse Cedex, France [email protected] *Corresponding Author Abstract The autonomy of spacecrafts can advantageously be enhanced by vision-based navigation (VBN) techniques. Applications range from manoeuvers around Solar System objects and landing on planetary surfaces, to in -orbit servicing or space debris removal, and even ground imaging. The development and validation of VBN algorithms for space exploration missions relies on the availability of physically accurate relevant images. Yet archival data from past missions can rarely serve this purpose and acquiring new data is often costly. Airbus has developed the image rendering software SurRender, which addresses the specific challenges of realistic image simulation with high level of representativeness for space scenes. In this paper we introduce the software SurRender and how its unique capabilities have proved successful for a variety of applications. Images are rendered by raytracing, which implements the physical principles of geometrical light propagation. Images are rendered in physical units using a macroscopic instrument model and scene objects reflectance functions. It is specially optimized for space scenes, with huge distances between objects and scenes up to Solar System size. Raytracing conveniently tackles some important effects for VBN algorithms: image quality, eclipses, secondary illumination, subpixel limb imaging, etc. From a user standpoint, a simulation is easily setup using the available interfaces (MATLAB/Simulink, Python, and more) by specifying the position of the bodies (Sun, planets, satellites, …) over time, complex 3D shapes and material surface properties, before positioning the camera. -
University Microfilms, a XEROX Company, Ann Arbor, Michigan
.72-4480 FAJEMIROKUN, Francis Afolabi, 1941- APPLICATION OF NEW OBSERVATIONAL SYSTEMS FOR SELENODETIC CONTROL. The Ohio State University, Ph.D., 1971 Geodesy University Microfilms, A XEROX Company, Ann Arbor, Michigan THIS DISSERTATION HAS BEEN MICROFILMED EXACTLY AS RECEIVED APPLICATION OF NEW OBSERVATIONAL SYSTEMS FOR SELENODETIC CONTROL DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University by Francis Afolabi Fajemirokun, B. Sc., M. Sc. The Ohio State University 1971 Approved by l/m /• A dviser Department of Geodetic Science PLEASE NOTE: Some Pages have indistinct p rin t. Filmed as received. UNIVERSITY MICROFILMS To Ijigbola, Ibeolayemi and Oladunni ACKNOW LEDGEME NTS The author wishes to express his deep gratitude to the many persons, without whom this work would not have been possible. First and foremost, the author is grateful to the Department of Geodetic Science and themembers of its staff, for the financial support and academic guidance given to him during his studies here. In particular, the author wishes to thank his adviser Professor Ivan I. Mueller, for his encouragement, patience and guidance through the various stages of this work. Professors Urho A. Uotila, Richard H. Rapp and Gerald H. Newsom served on the author’s reading committee, and offered many valuable suggestions to help clarify many points. The author has also enjoyed working with other graduate students in the department, especially with the group at 231 Lord Hall, where there was always an atmosphere of enthusiastic learning and of true friendship. The author is grateful to the various scientists outside the department, with whom he had discussions on the subject of this work, especially to the VLBI group at the Smithsonian Astrophysical Observatory in Cambridge, Ma s sachu s s etts . -
February 2014 BRAS Newsletter
February, 2014 Next Meeting February 10th 7PM at the HRPO Self Portrait of Mars Rover Opportunity: 10 years and still going! What's In This Issue? President's Message Vice-President's Message Secretary's Summary Message from HRPO Globe at Night 20/20 Vision Imagine Your Parks Recent Forum Posts President's Message Well, the Nordic ice giants have moved into the state and have settled in for a while. By the time you get this we will have gone through at least two episodes of wet icy sub- freezing weather fronts. We sorry Louisianans just are not used to this stuff. Thankfully, the skies are crystal clear afterwards. They aren’t always the best for planetary work, with the high atmospheric turbulence that often follows a front, but it is a good time for deep sky work. The skies provide a much higher contrast that allows us to see those fine low-contrast details that are often so hard to pull out in these climes. There is a supernova visible in the edge-on galaxy M82, in Ursa Major. As I write this, it is visible in scopes around 8 inches aperture and up, and easily photographed. Be sure to take a look. It is not every day we get a supernova so bright. During our last meeting, we took a vote on what item we BRAS members would like most as our next big ticket raffle prize. The Coronado PST won. They are much more affordable now, sometimes selling for as little as $650. We are shopping around for the best deal now. -
Water on the Moon, III. Volatiles & Activity
Water on The Moon, III. Volatiles & Activity Arlin Crotts (Columbia University) For centuries some scientists have argued that there is activity on the Moon (or water, as recounted in Parts I & II), while others have thought the Moon is simply a dead, inactive world. [1] The question comes in several forms: is there a detectable atmosphere? Does the surface of the Moon change? What causes interior seismic activity? From a more modern viewpoint, we now know that as much carbon monoxide as water was excavated during the LCROSS impact, as detailed in Part I, and a comparable amount of other volatiles were found. At one time the Moon outgassed prodigious amounts of water and hydrogen in volcanic fire fountains, but released similar amounts of volatile sulfur (or SO2), and presumably large amounts of carbon dioxide or monoxide, if theory is to be believed. So water on the Moon is associated with other gases. Astronomers have agreed for centuries that there is no firm evidence for “weather” on the Moon visible from Earth, and little evidence of thick atmosphere. [2] How would one detect the Moon’s atmosphere from Earth? An obvious means is atmospheric refraction. As you watch the Sun set, its image is displaced by Earth’s atmospheric refraction at the horizon from the position it would have if there were no atmosphere, by roughly 0.6 degree (a bit more than the Sun’s angular diameter). On the Moon, any atmosphere would cause an analogous effect for a star passing behind the Moon during an occultation (multiplied by two since the light travels both into and out of the lunar atmosphere). -
A Physically-Based Night Sky Model Henrik Wann Jensen1 Fredo´ Durand2 Michael M
To appear in the SIGGRAPH conference proceedings A Physically-Based Night Sky Model Henrik Wann Jensen1 Fredo´ Durand2 Michael M. Stark3 Simon Premozeˇ 3 Julie Dorsey2 Peter Shirley3 1Stanford University 2Massachusetts Institute of Technology 3University of Utah Abstract 1 Introduction This paper presents a physically-based model of the night sky for In this paper, we present a physically-based model of the night sky realistic image synthesis. We model both the direct appearance for image synthesis, and demonstrate it in the context of a Monte of the night sky and the illumination coming from the Moon, the Carlo ray tracer. Our model includes the appearance and illumi- stars, the zodiacal light, and the atmosphere. To accurately predict nation of all significant sources of natural light in the night sky, the appearance of night scenes we use physically-based astronomi- except for rare or unpredictable phenomena such as aurora, comets, cal data, both for position and radiometry. The Moon is simulated and novas. as a geometric model illuminated by the Sun, using recently mea- The ability to render accurately the appearance of and illumi- sured elevation and albedo maps, as well as a specialized BRDF. nation from the night sky has a wide range of existing and poten- For visible stars, we include the position, magnitude, and temper- tial applications, including film, planetarium shows, drive and flight ature of the star, while for the Milky Way and other nebulae we simulators, and games. In addition, the night sky as a natural phe- use a processed photograph. Zodiacal light due to scattering in the nomenon of substantial visual interest is worthy of study simply for dust covering the solar system, galactic light, and airglow due to its intrinsic beauty. -
Glossary of Lunar Terminology
Glossary of Lunar Terminology albedo A measure of the reflectivity of the Moon's gabbro A coarse crystalline rock, often found in the visible surface. The Moon's albedo averages 0.07, which lunar highlands, containing plagioclase and pyroxene. means that its surface reflects, on average, 7% of the Anorthositic gabbros contain 65-78% calcium feldspar. light falling on it. gardening The process by which the Moon's surface is anorthosite A coarse-grained rock, largely composed of mixed with deeper layers, mainly as a result of meteor calcium feldspar, common on the Moon. itic bombardment. basalt A type of fine-grained volcanic rock containing ghost crater (ruined crater) The faint outline that remains the minerals pyroxene and plagioclase (calcium of a lunar crater that has been largely erased by some feldspar). Mare basalts are rich in iron and titanium, later action, usually lava flooding. while highland basalts are high in aluminum. glacis A gently sloping bank; an old term for the outer breccia A rock composed of a matrix oflarger, angular slope of a crater's walls. stony fragments and a finer, binding component. graben A sunken area between faults. caldera A type of volcanic crater formed primarily by a highlands The Moon's lighter-colored regions, which sinking of its floor rather than by the ejection of lava. are higher than their surroundings and thus not central peak A mountainous landform at or near the covered by dark lavas. Most highland features are the center of certain lunar craters, possibly formed by an rims or central peaks of impact sites. -
A Spectroscopy Study of Nearby Late-Type Stars, Possible Members of Stellar Kinematic Groups
Astronomy & Astrophysics manuscript no. 14948 c ESO 2018 June 11, 2018 A spectroscopy study of nearby late-type stars, possible members of stellar kinematic groups ⋆ ⋆⋆ J. Maldonado1, R.M. Mart´ınez-Arn´aiz2 , C. Eiroa1, D. Montes2, and B. Montesinos3 1 Universidad Aut´onoma de Madrid, Dpto. F´ısica Te´orica, M´odulo 15, Facultad de Ciencias, Campus de Cantoblanco, E-28049 Madrid, Spain, 2 Universidad Complutense de Madrid, Dpto. Astrof´ısica, Facultad Ciencias F´ısicas, E-28040 Madrid, Spain 3 Laboratorio de Astrof´ısica Estelar y Exoplanetas, Centro de Astrobiolog´ıa, LAEX-CAB (CSIC-INTA), ESAC Campus, P.O. BOX 78, E-28691, Villanueva de la Ca˜nada, Madrid, Spain Received ; Accepted ABSTRACT Context. Nearby late-type stars are excellent targets for seeking young objects in stellar associations and moving groups. The origin of these structures is still misunderstood, and lists of moving group members often change with time and also from author to author. Most members of these groups have been identified by means of kinematic criteria, leading to an important contamination of previous lists by old field stars. Aims. We attempt to identify unambiguous moving group members among a sample of nearby-late type stars by studying their kinematics, lithium abundance, chromospheric activity, and other age-related properties. Methods. High-resolution echelle spectra (R ∼ 57000) of a sample of nearby late-type stars are used to derive accurate radial velocities that are combined with the precise Hipparcos parallaxes and proper motions to compute galactic-spatial velocity components. Stars are classified as possible members of the classical moving groups according to their kinematics. -
Digital Elevation Models of the Moon from Earth-Based Radar Interferometry Jean-Luc Margot, Donald B
1122 IEEE TRANSACTIONS ON GEOSCIENCE AND REMOTE SENSING, VOL. 38, NO. 2, MARCH 2000 Digital Elevation Models of the Moon from Earth-Based Radar Interferometry Jean-Luc Margot, Donald B. Campbell, Raymond F. Jurgens, Member, IEEE, and Martin A. Slade Abstract—Three-dimensional (3-D) maps of the nearside and of stereoscopic coverage. More recently, the Clementine space- polar regions of the Moon can be obtained with an Earth-based craft [7] carried a light detection and ranging (lidar) instrument, radar interferometer. This paper describes the theoretical back- which was used as an altimeter [1]. The lidar returned valid ground, experimental setup, and processing techniques for a se- quence of observations performed with the Goldstone Solar System data for latitudes between 79 S and 81 N, with an along-track Radar in 1997. These data provide radar imagery and digital ele- spacing varying between a few km and a few tens of km. The vation models of the polar areas and other small regions at IHH across track spacing was roughly 2.7 in longitude or 80 km m spatial and SH m height resolutions. A geocoding procedure at the equator. Because the instrument was somewhat sensitive relying on the elevation measurements yields cartographically ac- to detector noise and to solar background radiation, multiple re- curate products that are free of geometric distortions such as fore- shortening. turns were recorded for each laser pulse. An iterative filtering procedure selected 72 548 altimetry points for which the radial Index Terms—Interferometry, moon, radar, topography. error is estimated at 130 m [1]. -
Arxiv:2107.09416V1
Draft version July 21, 2021 A Typeset using L TEX twocolumn style in AASTeX631 Estimation of the Eclipse Solar Radius by Flash Spectrum Video Analysis Luca Quaglia,1 John Irwin,2 Konstantinos Emmanouilidis,3 and Alessandro Pessi4 1Sydney, New South Wales, Australia 2Guildford, England, United Kingdom 3Thessaloniki, Greece 4Milan, Italy ABSTRACT The value of the eclipse solar radius during the 2017 August 21st total solar eclipse was estimated to be S⊙ = (959.95±0.05)”at 1 au with no significant dependence on wavelength. The measurement was obtained from the analysis of a video of the eclipse flash spectrum recorded at the southern limit of the umbral shadow path. Our analysis was conducted by extracting light curves from the flash spectrum and comparing them to simulated light curves. Simulations were performed by integrating the limb darkening function (LDF) over the exposed area of photosphere. These numerical integrations relied upon very precise computations of the relative movement of the lunar and solar limbs. Keywords: Solar radius (1488) — Solar eclipses (1489) — Flash spectrum (541) — Light curves (918) — Astronomical simulations (1857) 1. INTRODUCTION rameters is now below the milliarcsecond level while the accuracy of UT1 determination is well below the mil- The value of the solar radius at unit distance S⊙ is one of the fundamental quantities needed to perform very lisecond level. Satellite missions in the last decade have precise eclipse computations. Some of the other required vastly improved the knowledge of the topography of the inputs are: accurate ephemerides for the position of the Moon (Smith et al. 2017) to better than 10 m (corre- centres of mass of the Sun and Moon; accurate models sponding to about 5 mas at the mean geocentric dis- for the orientation of the Earth and Moon; and detailed tance of the Moon), allowing accurate computations of data on the topography of the Moon and Earth. -
Characterizing the Radio Quiet Region Behind the Lunar Farside for Low Radio Frequency Experiments
Characterizing the Radio Quiet Region Behind the Lunar Farside for Low Radio Frequency Experiments Neil Bassetta,∗, David Rapettia,b,c, Jack O. Burnsa, Keith Tauschera,d, Robert MacDowalle aCenter for Astrophysics and Space Astronomy, Department of Astrophysical and Planetary Science, University of Colorado, Boulder, CO 80309, USA bNASA Ames Research Center, Moffett Field, CA 94035, USA cResearch Institute for Advanced Computer Science, Universities Space Research Association, Mountain View, CA 94043, USA dDepartment of Physics, University of Colorado, Boulder, CO 80309, USA eNASA Goddard Space Flight Center, Greenbelt, MD 20771, USA Abstract Low radio frequency experiments performed on Earth are contaminated by both ionospheric effects and radio frequency interference (RFI) from Earth-based sources. The lunar farside provides a unique environment above the ionosphere where RFI is heavily attenuated by the presence of the Moon. We present electrodynamics simulations of the propagation of radio waves around and through the Moon in order to characterize the level of attenuation on the farside. The simulations are performed for a range of frequencies up to 100 kHz, assuming a spherical lunar shape with an average, constant density. Additionally, we investigate the role of the topography and density profile of the Moon in the propagation of radio waves and find only small effects on the intensity of RFI. Due to the computational demands of performing simulations at higher frequencies, we propose a model for extrapolating the width of the quiet region above 100 kHz that also takes into account height above the lunar surface as well as the intensity threshold chosen to define the quiet region. -
INTERAGENCY REPORT: ASTROGEOLOGY 7 ADVANCED SYSTEMS TRAVERSE RESEARCH PROJECT REPORT by G
INTERAGENCY REPORT: ASTROGEOLOGY 7 ADVANCED SYSTEMS TRAVERSE RESEARCH PROJECT REPORT By G. E. Ulrich With a Section on Problems for Geologic Investigations of the Orientale Region of the Moon By R. S. Saunders July 1968 CONTENTS Page Abs tract . ............. 1 Introduct ion . •• # • ••• ••• .' • 2 Physiographic subdivision of the lunar surface 3 Site selection and preliminary traverse research. 8 Lunar topographic data •••••••.•.•••••• 17 Objectives and evaluation of traverse concepts • 20 Recommendations for continued traverse research .••• 26 Problems for geologic investigations of the Orientale region of the Moon, by R. S. Saunders 30 Introduct ion •.•• •••. 30 Physiography 30 Pre-Orbiter observations and i~terpretations 35 Geologic interpretations based on Orbiter photography ••••••••• 38 Conelusions •••• .•••. 54 References 56 ILLUSTRATIONS Figure 1. Map and index to photographs of Orientale basin region ••••.•••••• 4 2. Crater-size frequency distributions of Orientale basin terrain units •••••• 11 3. Orientale basin region showing pre- liminary traverse evaluation areas ••••• 14 4. Effect of photographic exposure on shadow measurements 15 5. Alternate traverse areas for short and intermediate duration missions. North eastern sector of central Orientale basin ................... 24 6. Preliminary photogeologic map of the Orientale basin region. .•• .. .. 32 iii Page Figure 7. Sketch map of Mare Orientale region prepared from Earth-based telescopic photography • 36 8-21. Orbiter IV photographs of Orientale basin region showing-- . 8. Part of wr{nk1e ridge . 41 9. Slump scarps around steptoe and collapse depression . 44 10. Slump scarps along margin of central mare basin outlining collapse depression • • . • 44 11. Possible caldera 45 12. Northeast quadrant of inner ring showing central basin material and mare units 45 13.