Microcraters in aluminum foils exposed by Stardust

Hörz F., Borg J., Bradley J. P., Bridges J., Brownlee D. E., Burchell M. J., Cole M. J., Dai Z. R., Djouadi Z., Floss C., Franchi I. A., Graham G. A., Green S. F., Heck P., Hoppe P., Kearsley A. T., Leitner J., Leroux H., Teslich N., Marhas K. K., Schwandt C. S., See T. H., Stadermann F. J., Stephan T., Troadec D., Tsou P., and Zolensky M. E. (2006)
Lunar Planet. Sci. XXXVII, Abstract #1148.


ABSTRACT

The Stardust Mission exposed some 1039 cm2 of aerogel and some 153 cm2 of aluminum-foil to the particle flux of comet Wild 2. The expected population of microcraters on these foils represents a substantial science opportunity, complementing the analysis of individual particles trapped in aerogel. Owing to the much higher shock stresses upon encounter of the dense aluminum foils, the projectile remnants residing in the bottom, walls, and rim area of these foil craters will be more severely altered, most likely molten and possibly vaporized, however, compared to those recovered from aerogel. Nevertheless, beginning with the investigation of multi-layer thermal blankets from the Solar Maximum Mission and extending into the Long Duration Exposure Facility, and more recent opportunities on space exposed surfaces, it was demonstrated that compositionally diverse particle types can be distinguished readily on aluminum (and other) substrates with modern analytical instruments.

In addition, the size frequency distribution and total flux of particles in the comets coma - using passive collector instruments that are returned to Earth - is much better determined with non-porous targets than with highly porous materials. Experimental evidence and empirical analyses of spaceexposed aerogels revealed that it is difficult, if not impractical, to extract the initial particle size or mass from either the detailed morphologic characteristics of a penetration track, or from the size of the trapped residue in aerogel. The physical cohesion of a prospective impactor (e.g., a single micro-crack) substantially controls the penetration outcome in aerogel, because projectiles of otherwise identical bulk-properties can fragment or completely disaggregate, producing dramatically different track morphologies that range from classical carrotshaped tracks to cylindrical cavities and bulbous pits. In contrast, the cratering flow fields and thus the morphology of small microcraters in non-porous targets are relatively invariant. As a consequence, the crater populations on the Stardust aluminum foils will become the primary features, vastly superior to penetration tracks, to deduce initial size or mass distributions and associated fluxes of the dust-particles encountered during Stardusts flyby of comet Wild 2. These determinations constitute the primary objective of the Stardust Cratering Team, and they will greatly complement the flux measurements of the active experiments on board the space craft.


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