CASSE — The ROSETTA Lander Comet Acoustic Surface Sounding Experiment — status of some aspects, the technical realisation and laboratory simulations
Introduction
After the successful space missions to comet 1P/Halley in 1986, experiments with “artificial comets” were made in the Space Simulator of the Institute of Space Simulation of DLR Cologne. This “Cometary Simulation” (KOSI, an acronym of the German expression “Kometensimulation”) programme, financially supported by the Deutsche Forschungsgemeinschaft, was performed from 1987 to 1993 (Kochan et al., 1999, Sears et al., 1999). The physical processes near and in the surface of the artificial comets were studied under simulated space conditions. The input parameters for the simulation were derived from results gathered by the Giotto mission to comet 1P/Halley and from Fred Whipple’s model of a “dirty snowball” (Whipple, 1950, Whipple, 1951), expressing the hypothesis that cometary nuclei consist mainly of a mixture of minerals and water ice. Comet 1P/Halley, taken as a prototype for all comets, consists of fluffy ice, comparable to dark velvet, with a density of around 0.3 g/cm3 and an albedo of 4% (Keller et al., 1987), although these numbers have been debated (Sagdeev et al., 1988, Colangeli et al., 1989, Peale, 1989, Rickman, 1989).
For the expected nature of the comet surface, it is very important to note that comet 46P/Wirtanen is of rather small size. Astronomical observations and model calculations indicate a radius of about 550 m (Jorda and Rickman, 1995, Cartwright et al., 1997, Benkhoff, 1999, Möhlmann, 1999). This might be a hint that 46P/Wirtanen, as a member of the Jupiter-family of short period comets, is in itself a building-block of a former larger body, remaining from earlier splits, or that it consists of only a few of such smaller building-blocks. This strengthens the interest in studying especially this comet and its internal structure. Such an experiment may provide deeper insight in the earlier growth processes in the preplanetary disk. The investigation of the nucleus’ structure will help to understand the processes of formation and origin of cometary nuclei (accretion from smaller bodies, disruption of parent bodies, homogeneous growth, etc.). Knowledge of the mechanical properties of the surface layers (in the dm- to m-range) is a key in understanding the evolution and future development of comet nuclei with respect to, e.g. outgassing, crustal formation, surface evolution, layering, increasing thickness of surface layers or quenching of outgassing, and especially the phenomenon of variable cometary activity, related to the volatile (water) budget of the surface layers. These data about the “pristine” composition will help to understand the origin and evolution of cometary nuclei. This is the main scientific objective of the ROSETTA mission and the Lander experiments. Furthermore, a detailed knowledge of the upper surface layers of the nucleus of P/46 Wirtanen will be a necessary prerequisite to derive the pristine composition and structure of this nucleus. The gases propagating from the sites, where they are released, are monitored by the Lander as well as by the orbiter. This gas emission is strongly influenced by the physical status of the upper surface layers.
Large cometary nuclei with a sufficiently strong gravitation are assumed to have a gravitationally-caused formation of at least local mantles or surface covers (Kührt and Keller, 1994, Möhlmann, 1994, Möhlmann, 1996a, Möhlmann, 1996b), formed out of the sublimation residua, the refractory material. Due to the small mass of comet 46P/Wirtanen, it is expected that its surface is made up mainly of a bare ice-crust.
In some parts of the cometary surface, e.g. in polar latitudes not irradiated by the sun, or even in valleys, regolith material may be accumulated, e.g. by avalanches (Grün et al., 1993). The surface and the subsurface region are expected to consist of layers, made up of hardened ice-mineral mixtures, with a cohesion ranging in hardness from a few kPa to some MPa, caused by sintering processes within the granular material and the recondensation of the different sublimated ice constituents. Our knowledge of the physical properties of cometary matter and the related structure of cometary nuclei is limited, and the nature of the interface between the feet of the Lander and the cometary surface is largely unknown. This requires the design of Lander feet which on one hand, ensures sufficient acoustic coupling to the cometary ground and on the other hand, it guarantees a safe landing without the danger that the Lander crashes on or into the ground.
To cope with the unknown mechanical conditions on and in the cometary surface, acoustic wave propagation experiments were made in various materials, to simulate different cometary conditions. Material analogues to regolithic dust and sand on one hand, and hardened ice dust mixtures on the other, were studied in the laboratory and in the outdoors. The technical design of the CASSE space experiment (Möhlmann, 1995) to be performed on comet Wirtanen requires extensive laboratory simulations and this paper reports some of these experiments.
Section snippets
The acoustic sounding experiment CASSE on board the ROSETTA Lander
In the context of ESA’s cornerstone mission ROSETTA (Schwehm and Langevin, 1991), destined for the first in situ inspection of a comet by a Lander, it was proposed to investigate the cometary surface layers by acoustic sounding. The ROSETTA mission scenario is made up by a spacecraft which carries a Lander piggyback. The spacecraft will be launched in 2003 and will have a rendezvous with comet 46P/Wirtanen in 2011 at a distance of around 4 AU from the Sun. The spacecraft will orbit the comet
Experiments
Physical parameters related to material properties include elastic parameters such as the Young’s modulus E and the Poisson ratio ν. They are related byto the velocities of the compression, cp, and shear waves, cs, respectively and to the bulk density ρ of the material. The elastic parameters above can be expressed in terms of other mechanical parameters, such as bulk modulus and rigidity and enter into other properties such as tensile strength. The wave
Discrimination of the arrival time of compression and shear waves
In a homogeneous and isotropic medium, two types of acoustic waves can propagate through a body, the compression wave and the shear wave, with velocities cp and cs, respectively. Surface waves are not considered here. Since cp>cs, the propagation time of the compression wave can easily be determined by the arrival of the first signal. The determination of the arrival time of shear waves is more difficult because of the superposition by the compression wave. A suitable positioning of the
Outdoor experiments with the Lander feet
During the first outdoor experiments in a testbed, filled with Rhine-sand, using the prototype piezo-stack transmitters, at least a distance of 2 m could be covered by acoustic wave propagation in a sand, cryogenised with liquid nitrogen. Improvements of the transmitting power of the piezo-stacks were achieved by matching the electrical impedance to the electronic transmitter and receiver, and by optimising the coupling piezoelectric actuator to the foot sole by transforming the small amplitude
Conclusions
Acoustic sounding of comet analog material was verified by laboratory and outdoor experiments. The acoustic sounding is well-suited to study mechanical and structural properties of sand, ice, and mineral samples under conditions similar to those on a cometary surface. Mechanical properties such as Young’s modulus E and Poisson’s ratio ν have been determined from measurements of wave velocities in sprayed ice, however, without admixed minerals, thus not completely simulating cometary relevant
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