| Literature DB >> 33222646 |
Armin Wedler1, Martin J Schuster1, Marcus G Müller1, Bernhard Vodermayer1, Lukas Meyer1, Riccardo Giubilato1, Mallikarjuna Vayugundla1, Michal Smisek1, Andreas Dömel1, Florian Steidle1, Peter Lehner1, Susanne Schröder2, Emanuel Staudinger3, Bernard Foing4, Josef Reill1.
Abstract
The Earth's moon is currently an object of interest of many space agencies for unmanned robotic missions within this decade. Besides future prospects for building lunar gateways as support to human space flight, the Moon is an attractive location for scientific purposes. Not only will its study give insight on the foundations of the Solar System but also its location, uncontaminated by the Earth's ionosphere, represents a vantage point for the observation of the Sun and planetary bodies outside the Solar System. Lunar exploration has been traditionally conducted by means of single-agent robotic assets, which is a limiting factor for the return of scientific missions. The German Aerospace Center (DLR) is developing fundamental technologies towards increased autonomy of robotic explorers to fulfil more complex mission tasks through cooperation. This paper presents an overview of past, present and future activities of DLR towards highly autonomous systems for scientific missions targeting the Moon and other planetary bodies. The heritage from the Mobile Asteroid Scout (MASCOT), developed jointly by DLR and CNES and deployed on asteroid Ryugu on 3 October 2018 from JAXA's Hayabusa2 spacecraft, inspired the development of novel core technologies towards higher efficiency in planetary exploration. Together with the lessons learnt from the ROBEX project (2012-2017), where a mobile robot autonomously deployed seismic sensors at a Moon analogue site, this experience is shaping the future steps towards more complex space missions. They include the development of a mobile rover for JAXA's Martian Moons eXploration (MMX) in 2024 as well as demonstrations of novel multi-robot technologies at a Moon analogue site on the volcano Mt Etna in the ARCHES project. Within ARCHES, a demonstration mission is planned from the 14 June to 10 July 2021,1 during which heterogeneous teams of robots will autonomously conduct geological and mineralogical analysis experiments and deploy an array of low-frequency antennas to measure Jovian and solar bursts. This article is part of a discussion meeting issue 'Astronomy from the Moon: the next decades'.Entities:
Keywords: ARCHES demonstration mission; Martian Moons eXploration (MMX); Mobile Asteroid Scout (MASCOT); planetary exploration; robotics
Year: 2020 PMID: 33222646 PMCID: PMC7739903 DOI: 10.1098/rsta.2019.0574
Source DB: PubMed Journal: Philos Trans A Math Phys Eng Sci ISSN: 1364-503X Impact factor: 4.226
Figure 1.(a,b) Artist impression of the MASCOT lander on Ryugu, photo of the MASCOT lander flight model; dimensions: 29 × 28 × 21 cm, weight: 10 kg. (Online version in colour.)
Figure 2.(a–c) ROBEX experiments at a Moon analogue site on Mt Etna: autonomous deployment of an array of seismic sensors housed in modular payload boxes with our Lightweight Rover Unit (LRU) rover prototype [15,16]. (Online version in colour.)
Figure 5.Graphical summary of the sequence of actions for LOFAR deployment on a Moon-like environment as part of the ARCHES demonstration mission. From top left to bottom right: (a) mission control denotes potential locations for the antenna array; (b) a drone scouts the target locations to assess the feasibility of deployment; (c) mission control defines final locations for the antenna array; (d) ground robots are sent to position the LOFAR boxes; (e) the antenna array is deployed and calibrated. The different grey marked areas (red and green online) denote optimal and sub-optimal locations for the incremental deployment of the next array elements, white arrows denote the movements of a robotic unit and dark (blue) markers are LOFAR boxes. The background image is a top-down view of the test site on Mt Etna, Sicily, where the ARCHES demo mission will take place. Note that the image is not drawn to scale but serves only for illustration purposes. (Online version in colour.)
Figure 3.(a,b) Scouting drone ARDEA [27] with the field of view of its stereo-vision multi-fisheye camera system. (Online version in colour.)
Figure 4.ScienceCam [20] with its left- and right wide-angle cameras (LWAC and RWAC) featuring colour- and narrow-band spectral filter wheels. (Online version in colour.)
Science Traceability Matrix for the ARCHES Demonstration Mission.
| scientific objectives | technological mean | systems/instruments involved | technical requirements and instrument specifications |
|---|---|---|---|
| observation of Jupiter and solar radio bursts | deployment of a low-frequency array radio telescope (LOFAR) calibration of the low frequency radio array localization of LOFAR antennas |
self-unfolding short dipole antennas embedded in payload boxes radio-CPT (communication, positioning and time-synchronization) ARDEA: inspection potential deployment areas LRU2: manipulation of sensor boxes | precise localization of each antenna of the array by radio communication, positioning and timing system (Radio-CPT). Positioning accuracy in order of 1/10 wavelength carrier frequency between 20 MHz and 30 MHz Deployment on an area of 100 × 100 m number of array elements 3 |
| elemental analysis of rock and sand samples | LIBS (Laser-induced breakdown spectroscopy) multi-spectral imaging (ScienceCam) | LIBS spectrometer embedded in payload boxes ARDEA: inspect potential areas regardless of traversability LRU: inspect terrain with spectral cameras (ScienceCam) to spot interesting targets LRU2: manipulation of payload boxes | LIBS Weight approximately 1 kg Nd: YAG laser wavelength 1064 nm with 8 mJ and 6 ns pulse LIBS spectrometer covers a range of wavelength of 550–770 nm detect hydrogen, silicon, calcium, sodium and potassium and more ScienceCam: 9 narrow-band filters (wavelengths of 450, 440, 660 nm and FERRIC filter set) mounted on pan-tilt unit |
Figure 6.Illustration of time scales of radio solar bursts variations in 16–28 MHz VLF range during 2 h (a), with a zoom of 20 mn on one event (b) (courtesy Paris Observatory Nancay Decametric Array). During the ARCHES campaign, after VLF functional proof of concept validation, we plan to measure such variations and track them in space and time. (Online version in colour.)
Figure 7.Image of Jupiter's radiation belts mapped from 13.8 MHz radio emission measured by the U.S. Cassini orbiter in January 2001 during its flyby of the planet. A superposed telescopic image of Jupiter to scale shows the size and orientation of the belts relative to the planet. Interpreted as synchrotron radiation, the emission delineates a doughnut-shaped region surrounding Jupiter where electrons moving near the speed of light radiate as they gyrate in the Jovian magnetic field. (Image courtesy NASA/JP). A lunar VLF radio interferometer can resolve the lobes and track the spatio-temporal variations of the lobes, in particular during Io induced radio bursts. (Online version in colour.)
Figure 8.(a,b) MMX Rover (Credit CNES); Mars, Phobos, Deimos (Credit: NASA); at PDR status, the Rover body is cuboid with dimensions of 38 cm × 23 cm and a weight of 29 kg. (Online version in colour.)