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The Formation of Encke Meteoroids and Dust Trail

✍ Scribed by William T. Reach; Mark V. Sykes; David Lien; John K. Davies


Publisher
Elsevier Science
Year
2000
Tongue
English
Weight
600 KB
Volume
148
Category
Article
ISSN
0019-1035

No coin nor oath required. For personal study only.

✦ Synopsis


We observed Comet 2P/Encke with the Infrared Space Observatory ISOCAM on July 14, 1997, from a particularly favorable viewing geometry above the comet's orbital plane and at a distance of 0.25 AU. A structured coma was observed, along with a long, straight dust trail. For the first time, we are able to observe the path of particles as they evolve from the nucleus to the trail. The particles that produce the infrared coma are large, with a radiation to gravitational force ratio Ξ² < 10 -3 (corresponding to >mmsized particles). The dust trail follows the orbit of the comet across our image, with a central core that is 2 Γ— 10 4 km wide, composed of particles with Ξ² < 10 -5 (size ∼5 cm) from previous apparitions. The abundant large particles near the comet pose a significant hazard to spacecraft. There is no evidence of a classical cometary dust tail due to small particles with Ξ² > 10 -3 , in marked contrast to other comets like P/Halley and C/Hale-Bopp. The structure of the coma requires anisotropic emission and requires that the spin axis of the nucleus be nearly parallel to the orbital plane, resulting in strong seasonal variations of the particle emission. While most of the infrared coma emission is due to dust produced during the 1997 apparition, the core of the dust trail requires emissions from previous apparitions. The total mass lost during the 1997 apparition is estimated to be 2-6 Γ— 10 13 g. Compared to the gas mass loss from ultraviolet observations, the dust-to-gas mass ratio is 10-30, much higher than has ever been suggested from visible light observations. Using the recently measured nuclear diameter, we find that Encke can last only 3000-10,000 ρ N yr 1 Based on observations with ISO, an ESA project with instruments funded by ESA member states (especially the PI countries: France, Germany, the Netherlands, and the United Kingdom) with the participation of ISAS and NASA.

(where ρ N is the nuclear density in g cm -3 ) at its present mass loss rate.


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