Surveyor and the Regolith 1966–1968
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Low-Energy Lunar Trajectory Design
LOW-ENERGY LUNAR TRAJECTORY DESIGN Jeffrey S. Parker and Rodney L. Anderson Jet Propulsion Laboratory Pasadena, California July 2013 ii DEEP SPACE COMMUNICATIONS AND NAVIGATION SERIES Issued by the Deep Space Communications and Navigation Systems Center of Excellence Jet Propulsion Laboratory California Institute of Technology Joseph H. Yuen, Editor-in-Chief Published Titles in this Series Radiometric Tracking Techniques for Deep-Space Navigation Catherine L. Thornton and James S. Border Formulation for Observed and Computed Values of Deep Space Network Data Types for Navigation Theodore D. Moyer Bandwidth-Efficient Digital Modulation with Application to Deep-Space Communication Marvin K. Simon Large Antennas of the Deep Space Network William A. Imbriale Antenna Arraying Techniques in the Deep Space Network David H. Rogstad, Alexander Mileant, and Timothy T. Pham Radio Occultations Using Earth Satellites: A Wave Theory Treatment William G. Melbourne Deep Space Optical Communications Hamid Hemmati, Editor Spaceborne Antennas for Planetary Exploration William A. Imbriale, Editor Autonomous Software-Defined Radio Receivers for Deep Space Applications Jon Hamkins and Marvin K. Simon, Editors Low-Noise Systems in the Deep Space Network Macgregor S. Reid, Editor Coupled-Oscillator Based Active-Array Antennas Ronald J. Pogorzelski and Apostolos Georgiadis Low-Energy Lunar Trajectory Design Jeffrey S. Parker and Rodney L. Anderson LOW-ENERGY LUNAR TRAJECTORY DESIGN Jeffrey S. Parker and Rodney L. Anderson Jet Propulsion Laboratory Pasadena, California July 2013 iv Low-Energy Lunar Trajectory Design July 2013 Jeffrey Parker: I dedicate the majority of this book to my wife Jen, my best friend and greatest support throughout the development of this book and always. -
Information Summaries
TIROS 8 12/21/63 Delta-22 TIROS-H (A-53) 17B S National Aeronautics and TIROS 9 1/22/65 Delta-28 TIROS-I (A-54) 17A S Space Administration TIROS Operational 2TIROS 10 7/1/65 Delta-32 OT-1 17B S John F. Kennedy Space Center 2ESSA 1 2/3/66 Delta-36 OT-3 (TOS) 17A S Information Summaries 2 2 ESSA 2 2/28/66 Delta-37 OT-2 (TOS) 17B S 2ESSA 3 10/2/66 2Delta-41 TOS-A 1SLC-2E S PMS 031 (KSC) OSO (Orbiting Solar Observatories) Lunar and Planetary 2ESSA 4 1/26/67 2Delta-45 TOS-B 1SLC-2E S June 1999 OSO 1 3/7/62 Delta-8 OSO-A (S-16) 17A S 2ESSA 5 4/20/67 2Delta-48 TOS-C 1SLC-2E S OSO 2 2/3/65 Delta-29 OSO-B2 (S-17) 17B S Mission Launch Launch Payload Launch 2ESSA 6 11/10/67 2Delta-54 TOS-D 1SLC-2E S OSO 8/25/65 Delta-33 OSO-C 17B U Name Date Vehicle Code Pad Results 2ESSA 7 8/16/68 2Delta-58 TOS-E 1SLC-2E S OSO 3 3/8/67 Delta-46 OSO-E1 17A S 2ESSA 8 12/15/68 2Delta-62 TOS-F 1SLC-2E S OSO 4 10/18/67 Delta-53 OSO-D 17B S PIONEER (Lunar) 2ESSA 9 2/26/69 2Delta-67 TOS-G 17B S OSO 5 1/22/69 Delta-64 OSO-F 17B S Pioneer 1 10/11/58 Thor-Able-1 –– 17A U Major NASA 2 1 OSO 6/PAC 8/9/69 Delta-72 OSO-G/PAC 17A S Pioneer 2 11/8/58 Thor-Able-2 –– 17A U IMPROVED TIROS OPERATIONAL 2 1 OSO 7/TETR 3 9/29/71 Delta-85 OSO-H/TETR-D 17A S Pioneer 3 12/6/58 Juno II AM-11 –– 5 U 3ITOS 1/OSCAR 5 1/23/70 2Delta-76 1TIROS-M/OSCAR 1SLC-2W S 2 OSO 8 6/21/75 Delta-112 OSO-1 17B S Pioneer 4 3/3/59 Juno II AM-14 –– 5 S 3NOAA 1 12/11/70 2Delta-81 ITOS-A 1SLC-2W S Launches Pioneer 11/26/59 Atlas-Able-1 –– 14 U 3ITOS 10/21/71 2Delta-86 ITOS-B 1SLC-2E U OGO (Orbiting Geophysical -
Radar Remote Sensing of Pyroclastic Deposits in the Southern Mare Serenitatis and Mare Vaporum Regions of the Moon Lynn M
JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 114, E11004, doi:10.1029/2009JE003406, 2009 Click Here for Full Article Radar remote sensing of pyroclastic deposits in the southern Mare Serenitatis and Mare Vaporum regions of the Moon Lynn M. Carter,1 Bruce A. Campbell,1 B. Ray Hawke,2 Donald B. Campbell,3 and Michael C. Nolan4 Received 21 April 2009; revised 12 July 2009; accepted 3 August 2009; published 5 November 2009. [1] We use polarimetric radar observations to study the distribution, depth, and embedded rock abundance of nearside lunar pyroclastic deposits. Radar images were obtained for Mare Vaporum and the southern half of Mare Serenitatis; the imaged areas contain the large Rima Bode, Mare Vaporum, Sulpicius Gallus, and Taurus-Littrow pyroclastic deposits. Potential pyroclastic deposits at Rima Hyginus crater, the Tacquet Formation, and a dome in Mare Vaporum are also included. Data were acquired at S band (12.6 cm wavelength) using Arecibo Observatory and the Green Bank Telescope in a bistatic configuration. The S band images have resolutions between 20 and 100 m/pixel. The pyroclastic deposits appear dark to the radar and have low circular polarization ratios at S band wavelengths because they are smooth, easily penetrable by radar waves, and generally contain few embedded blocks. Changes in circular polarization ratio (CPR) across some of the pyroclastic deposits show areas with increased rock abundance as well as deposits that are shallower. Radar backscatter and CPR maps are used to identify fine-grained mantling deposits in cases where optical and near-infrared data are ambiguous about the presence of pyroclastics. -
Photographs Written Historical and Descriptive
CAPE CANAVERAL AIR FORCE STATION, MISSILE ASSEMBLY HAER FL-8-B BUILDING AE HAER FL-8-B (John F. Kennedy Space Center, Hanger AE) Cape Canaveral Brevard County Florida PHOTOGRAPHS WRITTEN HISTORICAL AND DESCRIPTIVE DATA HISTORIC AMERICAN ENGINEERING RECORD SOUTHEAST REGIONAL OFFICE National Park Service U.S. Department of the Interior 100 Alabama St. NW Atlanta, GA 30303 HISTORIC AMERICAN ENGINEERING RECORD CAPE CANAVERAL AIR FORCE STATION, MISSILE ASSEMBLY BUILDING AE (Hangar AE) HAER NO. FL-8-B Location: Hangar Road, Cape Canaveral Air Force Station (CCAFS), Industrial Area, Brevard County, Florida. USGS Cape Canaveral, Florida, Quadrangle. Universal Transverse Mercator Coordinates: E 540610 N 3151547, Zone 17, NAD 1983. Date of Construction: 1959 Present Owner: National Aeronautics and Space Administration (NASA) Present Use: Home to NASA’s Launch Services Program (LSP) and the Launch Vehicle Data Center (LVDC). The LVDC allows engineers to monitor telemetry data during unmanned rocket launches. Significance: Missile Assembly Building AE, commonly called Hangar AE, is nationally significant as the telemetry station for NASA KSC’s unmanned Expendable Launch Vehicle (ELV) program. Since 1961, the building has been the principal facility for monitoring telemetry communications data during ELV launches and until 1995 it processed scientifically significant ELV satellite payloads. Still in operation, Hangar AE is essential to the continuing mission and success of NASA’s unmanned rocket launch program at KSC. It is eligible for listing on the National Register of Historic Places (NRHP) under Criterion A in the area of Space Exploration as Kennedy Space Center’s (KSC) original Mission Control Center for its program of unmanned launch missions and under Criterion C as a contributing resource in the CCAFS Industrial Area Historic District. -
Dsc Pub Edited
1968 93) few craters, much like the mare sites, Surveyor 7 although the general area was rougher. About Nation: U.S. (43) 21 hours after landing, ground controllers Objective(s): lunar soft-landing fired a pyrotechnic charge to drop the alpha- Spacecraft: Surveyor-G scattering instrument on the lunar surface. Spacecraft Mass: 1,040.1 kg When the instrument failed to move, con- Mission Design and Management: NASA JPL trollers used the robot arm to force it down. Launch Vehicle: Atlas-Centaur (AC-15 / Atlas The scoop on the arm was used numerous 3C no. 5903C / Centaur D-1A) times for picking up soil, digging trenches, Launch Date and Time: 7 January 1968 / and conducting at least sixteen surface- 06:30:00 UT bearing tests. Apart from taking 21,274 pho- Launch Site: ETR / launch complex 36A tographs (many of them in stereo), Surveyor Scientific Instruments: 7 also served as a target for Earth-based 1) imaging system lasers (of 1-watt power) to accurately 2) alpha-scattering instrument measure the distance between Earth and the 3) surface sampler Moon. Although it was successfully reacti- 4) footpad magnet vated after the lunar night, Surveyor 7 Results: Since Surveyors 1, 3, 5, and 6 success- finally shut down on 21 February 1968. In fully fulfilled requirements in support of total, the five successful Surveyors returned Apollo, NASA opted to use the last remaining more than 87,000 photos of the lunar surface Surveyor for a purely scientific mission out- and demonstrated the feasibility of soft- side of exploring a potential landing site for landing a spacecraft on the lunar surface. -
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). -
Rocket Plume Interactions for NASA Landing Systems
https://ntrs.nasa.gov/search.jsp?R=20200000979 2020-03-28T19:06:15+00:00Z National Aeronautics and Space Administration Rocket Plume Interactions for NASA Landing Systems December 4th 2019 Dr. Manish Mehta Aerosciences Branch NASA Marshall Space Flight Center marshallmarshall NASA – DLR Technical Interchange Meeting www.nasa.gov NASA Aerosciences Two main areas Agency makes it a commitment to fully investigate the performance and environments of their vehicles Rocket plume-induced environments Launch vehicle & upper-stage base flows Lander base flows Plume-induced flow separation (PIFS) Plume impingement Stage Separation Motors Attitude Control Motors Lander Leg Struts/Footpad Plume-Surface interactions (PSI) Erosion Physics Ejecta Dynamics Plume Physics Plume-induced aerodynamics Launch Vehicles Landing Systems Aerodynamic flow environments Earth crew vehicle re-entry flows Shuttle Orbiter Apollo Fuel/oxidizer tank, booster element earth re-entry External Tank, SRBs Launch vehicle ascent aerodynamic flow/heating Planetary spacecraft re-entry flows Mars Science Laboratory (MSL) 2 Concept – Plume Surface Interaction (PSI) PSI Definition: • Rocket plume-surface interaction (PSI) is a multi-phase and multi-system complex discipline that describes the lander environment due to the impingement of hot rocket exhaust on regolith of planetary bodies. This environment is characterized by the plume flow physics, cratering physics and ejecta dynamics. Problem Statement: • Extraterrestrial PSI cannot be accurately modeled with cold flow terrestrial testing. There are technical gaps in the physics modeling in the predictive simulation tools and ground tests. There are limited to no flight instrumentation dedicated to PSI. An accurate, validated predictive simulation capability is required to mitigate against lunar dust environments and to land large, heavy payloads. -
Apollo Over the Moon: a View from Orbit (Nasa Sp-362)
chl APOLLO OVER THE MOON: A VIEW FROM ORBIT (NASA SP-362) Chapter 1 - Introduction Harold Masursky, Farouk El-Baz, Frederick J. Doyle, and Leon J. Kosofsky [For a high resolution picture- click here] Objectives [1] Photography of the lunar surface was considered an important goal of the Apollo program by the National Aeronautics and Space Administration. The important objectives of Apollo photography were (1) to gather data pertaining to the topography and specific landmarks along the approach paths to the early Apollo landing sites; (2) to obtain high-resolution photographs of the landing sites and surrounding areas to plan lunar surface exploration, and to provide a basis for extrapolating the concentrated observations at the landing sites to nearby areas; and (3) to obtain photographs suitable for regional studies of the lunar geologic environment and the processes that act upon it. Through study of the photographs and all other arrays of information gathered by the Apollo and earlier lunar programs, we may develop an understanding of the evolution of the lunar crust. In this introductory chapter we describe how the Apollo photographic systems were selected and used; how the photographic mission plans were formulated and conducted; how part of the great mass of data is being analyzed and published; and, finally, we describe some of the scientific results. Historically most lunar atlases have used photointerpretive techniques to discuss the possible origins of the Moon's crust and its surface features. The ideas presented in this volume also rely on photointerpretation. However, many ideas are substantiated or expanded by information obtained from the huge arrays of supporting data gathered by Earth-based and orbital sensors, from experiments deployed on the lunar surface, and from studies made of the returned samples. -
50 Years of Dust on the Moon: from Apollo to Cheng'e-4
DUST ON THE MOON: FROM APOLLO TO CHENG’E-4 Prof. Brian J. O’Brien School of Physics, University of Western Australia [email protected] www.uwa.edu.au/people/brian.obrien Ph. 61 8 9387 3827 DAP2017 Boulder, Colorado 12 January 2017 Presented by courtesy of Dr William M. Farrell, GSFC LDAP2010: OVERVIEW BY O’BRIEN 1. 1st REVIEW OF DDE, TDS AND LEAM EXPTS 2. DDE: 8 DISCOVERIES O’Brien 1970-2009 3. TDS: FIRST MODERN DISCUSSION GOLD’s DISCOVERY OF COHESIVE FORCES IN 1971 4. LEAM: SUGGESTED ALTERNATIVE CAUSE AS NOISE BITS IN BURSTS, PERHAPS FROM EMI 5. FINAL O’B IN 2011 “BUT WHO WILL LISTEN?” 6. LADEE FINDINGS CONSISTENT WITH #3 + #4? COHESIVE FORCES OF LUNAR DUST SURFACE DUST ON MOON: MAJOR ITEMS SINCE LDAP2010 O’BRIEN 2010-16 CHENG’E-3 & CHENG’E-4 • 2011:O’BRIEN LDAP-2010 • CHENG’E-3 & YUTU doi:10.1016/j.pss.2011.04.016 • YUTU FIFTH LUNAR ROVER • 2013: LUNAR WEATHER AT • IN 2013 FIRST IN 40 YEARS 3 APOLLO SITES • MOVED 100m LUNAR DAY 1 http:dx.doi.org/10.1016/j.pss. • NO MOVEMENTS AFTER 1st 2013.1002/2013SW000978 SUNRISE: WHY NOT? • 2015: SUNRISE-DRIVEN GROUND-TRUTH FACTS • CHENG’E-4 (2018): dx.doi.org/10.1016/j.pss.2015 #1 PRIORITY CHANGED 2016 .09.018 TO LUNAR DUST STUDIES SUNRISE DRIVEN EFFECTS APOLLO 12 DUST SYNERGIES WITH 2 SOLAR DETECTOR DDE CELLS AT RIGHT ANGLES INVENTED 12/01/1966 1 VSCE VERTICAL SOLAR CELL FACES EAST (SUNRISE MAX) 2 HSC HORIZONTAL CELL FACING UP (NOON MAX.). -
OSIRIS-Rex Goes Asteroid Collecting
OSIRIS-REx Goes Asteroid Collecting — Scott Messenger, NASA Johnson Space Center OSIRIS-REx is NASA’s third New Frontiers mission, following the New Horizons mission, which completed a flyby of Pluto in 2015, and the Juno mission to orbit Jupiter, which has just begun science operations. The OSIRIS-REx mission’s primary objective is to collect pristine surface samples of a carbonaceous asteroid and return them to Earth for analysis. Carbonaceous asteroids and comets are considered to be L “primitive” bodies that have preserved remnants of the solar system starting materials. By studying them, scientists can learn about the origin and earliest evolution of the solar system. The OSIRIS-REx spacecraft was launched on September 8, 2016, beginning its two- year journey to asteroid 101955 Bennu (formerly designated 1999 RQ36). After more than one year of detailed remote observations, OSIRIS-REx will obtain surface samples and return them to Earth in September 2023. The OSIRIS-REx proposal, led by the late Dr. Michael J. Drake, was selected during the 2011 New Frontiers competition, and is now led by Dr. Dante Lauretta of the University of Arizona. The Pmission name OSIRIS-REx (an acronym for Origins, Spectral Interpretation, Resource Identification, Security, Regolith Explorer) embodies five objectives: (1) Origins: Return and analyze a sample of a carbonaceous asteroid; (2) Spectral Interpretation: Provide ground truth for remote observations of asteroids; (3) Resource Identification: Determine the mineral and chemical makeup of a near-Earth asteroid; (4) Security: Directly measure the non-gravitational force known as the Yarkovsky effect, which changes asteroidal orbits through its Iinteraction with sunlight; and (5) Regolith Explorer: Determine the properties of unconsolidated material that covers the asteroid surface. -
Controls on Lunar Basaltic Volcanic Eruption Structure and Morphology: 2 Gas Release Patterns in Sequential Eruption Phases 3 L
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Lancaster E-Prints 1 Controls on Lunar Basaltic Volcanic Eruption Structure and Morphology: 2 Gas Release Patterns in Sequential Eruption Phases 3 L. Wilson1,2 and J. W. Head2 4 1Lancaster Environment Centre, Lancaster University, Lancaster LA1 4YQ, UK 5 2Department of Earth, Environmental and Planetary Sciences, Brown University, Providence, RI 6 02912 USA 7 8 Key Points: 9 Relationships between a diverse array of lunar mare effusive and explosive volcanic 10 deposits and landforms have previously been poorly understood. 11 Four stages in the generation, ascent and eruption of magma and gas release patterns are 12 identified and characterized. 13 Specific effusive, explosive volcanic deposits and landforms are linked to these four 14 stages in lunar mare basalt eruptions in a predictive and integrated manner. 15 16 Abstract 17 Assessment of mare basalt gas release patterns during individual eruptions provides the basis for 18 predicting the effect of vesiculation processes on the structure and morphology of associated 19 features. We subdivide typical lunar eruptions into four phases: Phase 1, dike penetrates to the 20 surface, transient gas release phase; Phase 2, dike base still rising, high flux hawaiian eruptive 21 phase; Phase 3, dike equilibration, lower flux hawaiian to strombolian transition phase; Phase 4, 22 dike closing, strombolian vesicular flow phase. We show how these four phases of mare basalt 23 volatile release, together with total dike volumes, initial magma volatile content, vent 24 configuration and magma discharge rate, can help relate the wide range of apparently disparate 25 lunar volcanic features (pyroclastic mantles, small shield volcanoes, compound flow fields, 26 sinuous rilles, long lava flows, pyroclastic cones, summit pit craters, irregular mare patches 27 (IMPs) and ring moat dome structures (RMDSs)) to a common set of eruption processes. -
Electrostatic Dust Transport Effects on Shaping the Surface Properties of the Moon and Airless Bodies Across the Solar
Electrostatic Dust Transport Effects on Shaping the Surface Properties of the Moon and Airless Bodies across the Solar SystemCo-Authors: David T. Blewett, JHU-APL Xu Wang Georgiana Kramer, Planetary Science Institute Donald Barker, NASA JSC and Jacobs Technology Inc. Laboratory for Atmospheric and Space Physics Christine Hartzell, University of Maryland (LASP) Daoru Han, Missouri University of Science and NASA-SSERVI’s Institute for Modeling Plasmas, Technology Mihaly Horányi, University of Colorado – Boulder Atmospheres and Cosmic Dust Ian Garrick-Bethell, University of California, Santa Cruz (IMPACT) Hsing-Wen Hsu, University of Colorado – Boulder University of Colorado – Boulder Joseph Wang, University of Southern California Rhushik Chandrachud, Mumbai University Dev anshu Jha, MVJ College of Engineering Adrienne Dove, University of Central Florida Amara Graps, Planetary Science Institute White paper for the Decadal Survey on Planetary Science and Astrobiology 2023-2032 Panel on Mercury and the Moon Feb. 26, 2021 1 Unresolved Observation Puzzles related to Electrostatic Dust Transport 2 Plasma-Surface Interactions at Airless Bodies Halekas et al Dust particles on the regolith surface of airless bodies are charged, and may be mobilized, lofted and transported through electrostatic mechanisms. 3 Lunar Horizon Glow (LHG) First evidence observed by Surveyor 5, 6 and 7 Height < 30 cm, dust particles ~10 m in dia. Dust Deposition on Lunar Rocks Image by Chang’E-3 rover Criswell, 1973; Rennilson & Criswell, 1974; Colwell et al., Yan et al., 2019 2007 Dust deposition is found to be up to ~28 cm high on the rocks, which is a similar height to the LHG 4 Apollo Observations Low-Speed Dust Detections at Terminator High-altitude Global LHG and Streamers by the Lunar Ejecta and Meteorites (LEAM) experiment (Sketches by Apollo 17 commander E.A.