日本地球惑星科学連合2023年大会

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[E] 口頭発表

セッション記号 P (宇宙惑星科学) » P-PS 惑星科学

[P-PS03] 太陽系小天体:太陽系の形成と進化における最新成果と今後の展望

2023年5月24日(水) 15:30 〜 16:45 301A (幕張メッセ国際会議場)

コンビーナ:岡田 達明(宇宙航空研究開発機構宇宙科学研究所)、吉田 二美(産業医科大学)、荒川 創太(海洋研究開発機構)、深井 稜汰(宇宙航空研究開発機構)、座長:吉田 二美(産業医科大学)、岡田 達明(宇宙航空研究開発機構宇宙科学研究所)、荒川 創太(海洋研究開発機構)、深井 稜汰(宇宙航空研究開発機構)


16:00 〜 16:15

[PPS03-20] Ejecta plume evolution observed in the Hayabusa2 impact experiment on Ryugu

*菊地 翔太1和田 浩二2白井 慶3石橋 高2門野 敏彦4本田 理恵5横田 康弘6嶌生 有理6坂谷 尚哉7小川 和律6、澤田 弘崇6荒川 政彦3 (1.国立天文台、2.千葉工業大学、3.神戸大学、4.産業医科大学、5.愛媛大学、6.宇宙航空研究開発機構、7.立教大学)

キーワード:小惑星、衝突イジェクタ、スケーリング則

Impact cratering is one of the most fundamental geological processes in planetary formation. The resultant particle ejection contributes to either resurfacing through the accretion process or interplanetary material transport as a consequence of ballistic escape. A number of experimental and numerical studies have therefore been conducted to characterize the dynamical evolution of impact ejecta. Nevertheless, their validities have rarely been tested in actual space environments. Against this background, Hayabusa2 conducted an impact experiment on the asteroid Ryugu in 2019.

In this experiment, a small carry-on impactor (SCI) was released from the spacecraft, firing a 2-kg liner at a velocity of 2 km/s. Previous research found that an artificial crater with an apparent diameter of 14.5 m was formed in the gravity-dominated regime [1]. In this study, we expanded our research to reconstruct the evolution of the ejecta plume produced by the SCI impact, relying on optical images obtained by Hayabusa2’s deployable camera (DCAM3) [2]. The dynamics of impact ejecta was investigated via two different approaches: the shape estimation of the ejecta curtain and the trajectory estimation of ejected boulders.

In the former analysis, we determined the velocity distribution of SCI ejecta by comparing the observed profile of the ejecta curtain and the theoretical model for gravity scaling. The major finding was that the material constants associated with ejecta scaling laws coincide with those of the typical sand target, μ = 0.41 and C2 = 0.64 [3], within their error ranges. The ejection angle of ejecta particles increased from approximately 35 to 50 deg in accordance with the distance from the SCI impact point. Although the angle and distance correlation was opposite to that of many on-ground experiments, the discrepancy can be well explained by the effects of oblique impact [4] and/or surface undulation. Combining the obtained results and the mathematical model describing subsurface excavation flows (Z-model), we further constrained the total mass excavated by the SCI impact and the fraction of particles that escaped from the asteroid.

The latter analysis aimed to determine the trajectories of decimeter-sized boulders observed as individual bright spots in DCAM3 images [5]. We successfully estimated the three-dimensional trajectories of four ejected boulders from 5–10 images. These boulders were ejected in the northeast to southeast directions. The surface-relative launch velocities were estimated to be approximately 20–30 cm/s, which were small enough for the boulders to return to the surface of Ryugu. The ejection angles of these boulders lay between 35 and 55 deg and were close to those of fine particles composing the ejecta curtain.

The ejecta evolution models constructed through this research could serve as a reference for future on-ground experiments and other space missions such as DART/Hera.

[1] Arakawa et al. (2020) Science, 368, 67-71.
[2] Wada et al. (2021) Astronomy and Astrophysics, 647, A43.
[3] Housen & Holsapple (2011) Icarus, 211, 865-875.
[4] Richardson et al. (2007) Icarus, 191, 176-209.
[5] Kadono et al. (2020) The Astrophysical Journal Letters, 899, L22.