Japan Geoscience Union Meeting 2015

Presentation information

Oral

Symbol P (Space and Planetary Sciences) » P-PS Planetary Sciences

[P-PS21] Planetary Sciences

Mon. May 25, 2015 11:00 AM - 12:45 PM A02 (APA HOTEL&RESORT TOKYO BAY MAKUHARI)

Convener:*Kosuke Kurosawa(Planetary Exploration Research Center, Chiba Institute of Technology), Keiko Hamano(Department of Earth and Planetary Science, Graduate School of Science, University of Tokyo), Chair:Shunichi Kamata(Department of Earth and Planetary Science, Graduate School of Science, The University of Tokyo), Shintaro Azuma(Department of Earth and Planetary Sciences System,Hiroshima university)

12:30 PM - 12:33 PM

[PPS21-P17] Thermal evolution simulation of asteroid Vesta

3-min talk in an oral session

*Tatsuhiko NOGAMI1, Sin-iti SHIRONO1 (1.Division of earth and planetary science, Nagoya univercity)

Vesta has been regarded as the parent body of the HED meteorites. From the observation of DAWN spacecraft, the uppermost layer of Vesta is composed from howardite ranging from 50km to 80km (Jutzi et al. 2013). It is known that the ratio of the number of eucrites to diogenites is around two. Based on these facts, rapidly cooled magma layer on Vesta should be more than 10km in thickness.
In this work, I studied the evolution of internal thermal evolution of Vesta due to heating of decay of 26Al. I calculate the temperature distribution by solving numerically heat conduction equation. According to Formisano et al.(2013), if Vesta completed its formation within 1.4Ma from the injections of 26Al into the solar nebula, the degree of silicate melting of inside Vesta exceeds 50 vol%. But in that work, convection and melt migration were not taken into account. These two mechanisms contribute to cool Vesta. So it is expected that the formation of Vesta is completed more early if these are taken into account. By the way, it is known that it takes about a few hundreds year for Vesta-size planet to complete its formation in planetary formation standard model.
As a convection model, I adopted the simple model of Kaula (1979). It was assumed that generated melt migrates the surface instantaneously, and the migrating melt to the surface was accounted as the rapidly cooled magma. There are two parameters in this study, including a (the percentage of melt migration) and t0 (formation time of Vesta), and perform simulation taking into account the convection and melt migration.
As a result, convection and melt migration substantially change the evolution of internal thermal structure, and total eruptive volume of melt considerably depends on a and t0. The magma volume increases as a increases. On the other hand, the magma volume decreases as t0 increases.
When t0=0, corresponding to no decay of 26Al at the beginning, and a>0.3, the erupting magma layer of 10km in thickness is formed. When a=1, that is all melt is erupted, the erupting magma layer of 10km is formed if t0<0.9Ma. According to these results, Vesta should be completed its formation within 0.9Ma after CAI formation, and more than 30% of generated melt should migrate the surface. But all generated melts aren't necessarily erupted, and if a<1, Vesta has to be completed more early.
Therefore, it is suggested that the formation time of Vesta should be more early than the estimate by Formisano et al.(2013), and that planetary formation standard model might have to be reviewed.