Geological Observations from Lunar Orbit R
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DMAAC – February 1973
LUNAR TOPOGRAPHIC ORTHOPHOTOMAP (LTO) AND LUNAR ORTHOPHOTMAP (LO) SERIES (Published by DMATC) Lunar Topographic Orthophotmaps and Lunar Orthophotomaps Scale: 1:250,000 Projection: Transverse Mercator Sheet Size: 25.5”x 26.5” The Lunar Topographic Orthophotmaps and Lunar Orthophotomaps Series are the first comprehensive and continuous mapping to be accomplished from Apollo Mission 15-17 mapping photographs. This series is also the first major effort to apply recent advances in orthophotography to lunar mapping. Presently developed maps of this series were designed to support initial lunar scientific investigations primarily employing results of Apollo Mission 15-17 data. Individual maps of this series cover 4 degrees of lunar latitude and 5 degrees of lunar longitude consisting of 1/16 of the area of a 1:1,000,000 scale Lunar Astronautical Chart (LAC) (Section 4.2.1). Their apha-numeric identification (example – LTO38B1) consists of the designator LTO for topographic orthophoto editions or LO for orthophoto editions followed by the LAC number in which they fall, followed by an A, B, C or D designator defining the pertinent LAC quadrant and a 1, 2, 3, or 4 designator defining the specific sub-quadrant actually covered. The following designation (250) identifies the sheets as being at 1:250,000 scale. The LTO editions display 100-meter contours, 50-meter supplemental contours and spot elevations in a red overprint to the base, which is lithographed in black and white. LO editions are identical except that all relief information is omitted and selenographic graticule is restricted to border ticks, presenting an umencumbered view of lunar features imaged by the photographic base. -
Cratering Flow Fields
Proc. Lunar Planet. Sci. Conj. !Ith (1980), p. 2347-2378. Printed in the United States of America 1980LPSC...11.2347C Cratering flow fields: Implications for the excavation and transient expansion stages of crater formation Steven Kent Croft Lunar and Planetary Institute, 3303 NASA Road I, Houston, Texas 77058 Abstract-A Maxwell Z-model cratering flow field originating at non-zero depths-of-burst has been used to calculate theoretical depths and volumes of excavation, hinge radii, ejection angles, and transient structural rim uplifts for comparison with experimental and field data from impact and explosion craters. The model flow fields match the observed data well for values of Z between 2.5 and 3.0 for both explosion and impact craters, and effective depths-of-burst near one projectile di- ameter for impacts. The model flow field is therefore inferred to be a reasonable first-order quantitative approximation for several important crater structures, and to embody the important qualitative fea- tures of impact and explosion cratering flows. Formation of a hinge about which the coherent ejecta flap rotates at the rim of the transient crater divides material in the flow field into ejected and down- ward and outward-driven portions. Ejected material originates from an excavation cavity which has a geometry distinct from the transient crater. The excavation cavity and transient crater have the same diameter, D1c, but the depth of the excavation cavity is -0. I D1c, or about one-third of the transient crater depth, and, in the case of simple bowl-shaped craters, about one-half the depth of the final apparent crater. -
October 2006
OCTOBER 2 0 0 6 �������������� http://www.universetoday.com �������������� TAMMY PLOTNER WITH JEFF BARBOUR 283 SUNDAY, OCTOBER 1 In 1897, the world’s largest refractor (40”) debuted at the University of Chica- go’s Yerkes Observatory. Also today in 1958, NASA was established by an act of Congress. More? In 1962, the 300-foot radio telescope of the National Ra- dio Astronomy Observatory (NRAO) went live at Green Bank, West Virginia. It held place as the world’s second largest radio scope until it collapsed in 1988. Tonight let’s visit with an old lunar favorite. Easily seen in binoculars, the hexagonal walled plain of Albategnius ap- pears near the terminator about one-third the way north of the south limb. Look north of Albategnius for even larger and more ancient Hipparchus giving an almost “figure 8” view in binoculars. Between Hipparchus and Albategnius to the east are mid-sized craters Halley and Hind. Note the curious ALBATEGNIUS AND HIPPARCHUS ON THE relationship between impact crater Klein on Albategnius’ southwestern wall and TERMINATOR CREDIT: ROGER WARNER that of crater Horrocks on the northeastern wall of Hipparchus. Now let’s power up and “crater hop”... Just northwest of Hipparchus’ wall are the beginnings of the Sinus Medii area. Look for the deep imprint of Seeliger - named for a Dutch astronomer. Due north of Hipparchus is Rhaeticus, and here’s where things really get interesting. If the terminator has progressed far enough, you might spot tiny Blagg and Bruce to its west, the rough location of the Surveyor 4 and Surveyor 6 landing area. -
THE STUDY of SATURN's RINGS 1 Thesis Presented for the Degree Of
1 THE STUDY OF SATURN'S RINGS 1610-1675, Thesis presented for the Degree of Doctor of Philosophy in the Field of History of Science by Albert Van Haden Department of History of Science and Technology Imperial College of Science and Teohnology University of London May, 1970 2 ABSTRACT Shortly after the publication of his Starry Messenger, Galileo observed the planet Saturn for the first time through a telescope. To his surprise he discovered that the planet does.not exhibit a single disc, as all other planets do, but rather a central disc flanked by two smaller ones. In the following years, Galileo found that Sa- turn sometimes also appears without these lateral discs, and at other times with handle-like appendages istead of round discs. These ap- pearances posed a great problem to scientists, and this problem was not solved until 1656, while the solution was not fully accepted until about 1670. This thesis traces the problem of Saturn, from its initial form- ulation, through the period of gathering information, to the final stage in which theories were proposed, ending with the acceptance of one of these theories: the ring-theory of Christiaan Huygens. Although the improvement of the telescope had great bearing on the problem of Saturn, and is dealt with to some extent, many other factors were in- volved in the solution of the problem. It was as much a perceptual problem as a technical problem of telescopes, and the mental processes that led Huygens to its solution were symptomatic of the state of science in the 1650's and would have been out of place and perhaps impossible before Descartes. -
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). -
APOLLO 15 OBSERVATIONS; Farouk El-Baz, Lunar Explora- Tion Department, Bellcomm, Washington, D.C
APOLLO 15 OBSERVATIONS; Farouk El-Baz, Lunar Explora- tion Department, Bellcomm, Washington, D.C. 20024; A. M. Worden and V. D. Brand, Astronaut Office, Manned Spacecraft Center, Houston, Texas 77058 Visual observations from lunar orbit constitute a signif- icant complement to photography and other remote-sensed data. Utilization of the capabilities of a well-trained observer in lunar orbit is an illustration of the role of man in space flight. This is particularly significant when one considers the special characteristics of the human eye and the interpretive powers of the brain. The unaided eye resolves 20-30 m objects from 110 km orbit. It is also especially equipped, through its wide dynamic range, to distinguish subtle differences in bright- ness levels, color tones, topographic expressions and textural variations. Fifteen lunar surface areas were studied in detail from lunar orbit on Apollo 15. The wide field of view allowed in- vestigation of both the general and local settings at varying sun elevation angles and viewing directions. "On the scene" interpretations were made and later checked and confirmed on successive orbits. In certain cases, features and phenomena were compared to similar occurrences in other parts of the groundtracks. Results of the observation of eight targets are given and an example is provided of the geologic significance of observing cinder cones on the southeastern rim of Mare Serenitatis. The more significant observations were made of the following features starting with the most easterly target: 1) Swirls of light colored markings on the floor of Mare Inginii on the lunar farside. No topographic expressions are associated with these sinuous markings which appear to have been the result of a "bleaching" mechanism. -
Lick Observatory Records: Photographs UA.036.Ser.07
http://oac.cdlib.org/findaid/ark:/13030/c81z4932 Online items available Lick Observatory Records: Photographs UA.036.Ser.07 Kate Dundon, Alix Norton, Maureen Carey, Christine Turk, Alex Moore University of California, Santa Cruz 2016 1156 High Street Santa Cruz 95064 [email protected] URL: http://guides.library.ucsc.edu/speccoll Lick Observatory Records: UA.036.Ser.07 1 Photographs UA.036.Ser.07 Contributing Institution: University of California, Santa Cruz Title: Lick Observatory Records: Photographs Creator: Lick Observatory Identifier/Call Number: UA.036.Ser.07 Physical Description: 101.62 Linear Feet127 boxes Date (inclusive): circa 1870-2002 Language of Material: English . https://n2t.net/ark:/38305/f19c6wg4 Conditions Governing Access Collection is open for research. Conditions Governing Use Property rights for this collection reside with the University of California. Literary rights, including copyright, are retained by the creators and their heirs. The publication or use of any work protected by copyright beyond that allowed by fair use for research or educational purposes requires written permission from the copyright owner. Responsibility for obtaining permissions, and for any use rests exclusively with the user. Preferred Citation Lick Observatory Records: Photographs. UA36 Ser.7. Special Collections and Archives, University Library, University of California, Santa Cruz. Alternative Format Available Images from this collection are available through UCSC Library Digital Collections. Historical note These photographs were produced or collected by Lick observatory staff and faculty, as well as UCSC Library personnel. Many of the early photographs of the major instruments and Observatory buildings were taken by Henry E. Matthews, who served as secretary to the Lick Trust during the planning and construction of the Observatory. -
Apollo 17 Index
Preparation, Scanning, Editing, and Conversion to Adobe Portable Document Format (PDF) by: Ronald A. Wells University of California Berkeley, CA 94720 May 2000 A P O L L O 1 7 I N D E X 7 0 m m, 3 5 m m, A N D 1 6 m m P H O T O G R A P H S M a p p i n g S c i e n c e s B r a n c h N a t i o n a l A e r o n a u t i c s a n d S p a c e A d m i n i s t r a t i o n J o h n s o n S p a c e C e n t e r H o u s t o n, T e x a s APPROVED: Michael C . McEwen Lunar Screening and Indexing Group May 1974 PREFACE Indexing of Apollo 17 photographs was performed at the Defense Mapping Agency Aerospace Center under the direction of Charles Miller, NASA Program Manager, Aerospace Charting Branch. Editing was performed by Lockheed Electronics Company, Houston Aerospace Division, Image Analysis and Cartography Section, under the direction of F. W. Solomon, Chief. iii APOLLO 17 INDEX 70 mm, 35 mm, AND 16 mm PHOTOGRAPHS TABLE OF CONTENTS Page INTRODUCTION ................................................................................................................... 1 SOURCES OF INFORMATION .......................................................................................... 13 INDEX OF 16 mm FILM STRIPS ........................................................................................ 15 INDEX OF 70 mm AND 35 mm PHOTOGRAPHS Listed by NASA Photograph Number Magazine J, AS17–133–20193 to 20375......................................... -
February 2019 Plato a to B
A PUBLICATION OF THE LUNAR SECTION OF THE A.L.P.O. EDITED BY: Wayne Bailey [email protected] 17 Autumn Lane, Sewell, NJ 08080 RECENT BACK ISSUES: http://moon.scopesandscapes.com/tlo_back.html FEATURE OF THE MONTH – FEBRUARY 2019 PLATO A TO B Sketch and text by Robert H. Hays, Jr. - Worth, Illinois, USA December 18, 2018 02:04-02:42, 02:58-03:10 UT, 15 cm refl, 170x, seeing 7-9/10, transparence 6/6. I observed the group of craters just west of Plato on the evening of Dec. 17/18, 2018. Plato A is the largest crater in this sketch. Three other craters form nearly a straight line to the west. From east to west, these are Plato M, Y and B. These four craters probably do not make a related chain since they differ considerably in appearance. Plato A has an irregular east rim (shadowed here) that appears to merge into an old ring. A small peak is near this old ring. Plato A also had a detached strip of internal shadow and substantial exterior shadow at this time. Plato M and Y look similar, but M seems deeper than Y. Plato M also had much exterior shadow. Plato B is the second largest crater depicted here, but it is shallower than its neighbors. Plato BA is the small crater northwest of Plato Y, and a small peak is farther to the northwest. A short ridge is just north of Plato Y. A large peak is northeast of Plato M, and Plato S is the crater far- ther northeast. -
Crater Size-Frequency Distribution Measurements of Mare Crisium
42nd Lunar and Planetary Science Conference (2011) 2179.pdf CRATER SIZE-FREQUENCY DISTRIBUTION MEASUREMENTS OF MARE CRISIUM. H. Hiesinger1, C. H. van der Bogert1, D. Reiss1, and M. S. Robinson2, 1Institut für Planetologie, Westfälische Wilhelms- Universität, Wilhelm-Klemm-Str. 10, 48149 Münster, Germany ([email protected]), 2Arizona State Uni- versity, Tempe, AZ, USA. Introduction: Mare Crisium is located between region of the basin was also mapped as Eratosthenian 10° and 30º N and 50° and 70º E on the lunar nearside. or Imbrian basalts (EIm). This unit roughly corre- Previous work [1] identified three major basalt groups sponds to the Group I basalts of [1]. The geologic map within the basin (Fig. 1). The soils formed from a Fe- of [3] also shows mostly Imbrian ages for the mare and Mg-rich high Ti basalt similar to Luna 16 samples basalts in southern Mare Crisium, except for two (Group I), a very low Ti ferrobasalt similar to Luna 24 small, isolated areas east of Picard X, which were samples (Group II), and a low Ti ferrobasalt similar to mapped as Eratosthenian or Imbrian basalts (EIm). Apollo 12 samples (Group III). Group I basalts appear Radiometric ages of the Luna 24 samples indicate ages to be the oldest deposits in the basin, as they are only of 3.34 to 3.44 Ga [4] or 2.52-3.45 Ga [5]. Crater deg- exposed in the topographically higher SE region of the radation ages of [6] show an age of 3.50 Ga for the basin and are excavated by major post-mare impact Luna 24 landing site (Fig. -
Arxiv:0706.3947V1
Transient Lunar Phenomena: Regularity and Reality Arlin P.S. Crotts Department of Astronomy, Columbia University, Columbia Astrophysics Laboratory, 550 West 120th Street, New York, NY 10027 ABSTRACT Transient lunar phenomena (TLPs) have been reported for centuries, but their nature is largely unsettled, and even their existence as a coherent phenomenon is still controversial. Nonetheless, a review of TLP data shows regularities in the observations; a key question is whether this structure is imposed by human observer effects, terrestrial atmospheric effects or processes tied to the lunar surface. I interrogate an extensive catalog of TLPs to determine if human factors play a determining role in setting the distribution of TLP reports. We divide the sample according to variables which should produce varying results if the determining factors involve humans e.g., historical epoch or geographical location of the observer, and not reflecting phenomena tied to the lunar surface. Specifically, we bin the reports into selenographic areas (300 km on a side), then construct a robust average count for such “pixels” in a way discarding discrepant counts. Regardless of how we split the sample, the results are very similar: roughly 50% of the report count originate from the crater Aristarchus and vicinity, 16% from Plato, 6% from recent, major impacts (Copernicus, ∼ ∼ Kepler and Tycho - beyond Aristarchus), plus a few at Grimaldi. Mare Crisium produces a robust signal for three of five averages of up to 7% of the reports (however, Crisium subtends more than one pixel). The consistency in TLP report counts for specific features on this list indicate that 80% of the reports arXiv:0706.3947v1 [astro-ph] 27 Jun 2007 ∼ are consistent with being real (perhaps with the exception of Crisium). -
EPSC-DPS2011-1095, 2011 EPSC-DPS Joint Meeting 2011 C Author(S) 2011
EPSC Abstracts Vol. 6, EPSC-DPS2011-1095, 2011 EPSC-DPS Joint Meeting 2011 c Author(s) 2011 Absolute model ages of basalts in Mare Crisium H. Hiesinger (1), C. H. van der Bogert (1), D. Reiss (1), and M. S. Robinson (2) (1) Institut für Planetologie, Westfälische Wilhelms-Universität, Wilhelm-Klemm-Str. 10, 48149 Münster, Germany, [email protected], (2) Arizona State University, Tempe, AZ, USA. Abstract presumably emplaced in two stages - first, around the We have dated several mare basalt units in Mare NE (Eimmart Basalts) and SE (Agarum Basalts) Crisium. On the basis of our crater size-frequency outer edge of the basin (Group IIB), and then in the distribution measurements (CSFD), we find Imbrian NNW of the basin (Group IIA; Swift Basalts). There and Eratosthenian ages for the investigated basalts. are several small occurrences of Group IIA Swift Basalts in the S, the easternmost of which contains 1. Introduction the Luna 24 landing site [1]. Group III basalts Mare Crisium is one of the most prominent lunar (Shapley Basalts) are the youngest basalts and are basins, located on the eastern nearside. According to exposed in the SSE of the basin. [1, 2], there are three major basalt groups within the While stratigraphic relationships among the Mare basin, i.e., an Fe- and Mg-rich high Ti basalt similar Crisium basalts were investigated in detail [e.g., 1], to Luna 16 samples (Group I), a very low Ti absolute and relative ages remain under discussion. ferrobasalt similar to Luna 24 samples (Group II), For example, the geologic map of [4] indicates that and a low Ti ferrobasalt similar to Apollo 12 samples most of northern Mare Crisium is covered by (Group III) (Fig.