[S-EM18] 地磁気・古地磁気・岩石磁気

[SEM18-14] Numerical modeling of a lunar dynamo and its long-term evolution

*兵藤 史¹、高橋 太²、金嶋 聰²、清水 久芳³、綱川 秀夫⁴ (1.九州大学大学院理学府地球惑星科学専攻、2.九州大学大学院理学研究院地球惑星科学部門、3.東京大学地震研究所、4.東京工業大学理学院地球惑星科学系)

キーワード：月のダイナモ、月の磁場、月の進化、熱史、内核成長、組成対流

Now the Moon has no global magnetic field unlike the Earth, and there are only local crustal fields which are of approximately several hundred nT on the lunar surface [Tsunakawa et al., 2015]. However, lunar paleomagnetic studies indicate evidence for ancient lunar dynamo, and that the Moon had a global magnetic field of about 70 μT on the lunar surface at least between 4.2 and 3.56 Ga [e.g., Garrick-Bethell et al. 2009; Shea et al., 2012; Suavet et al., 2013]. In this study, we assume that the lunar dynamo is powered by compositional buoyancy due to inner core growth, which enabled the dynamo to work for such a long time interval. Based on the assumption, we perform a series of numerical simulations of MHD dynamo by varying the ratio of the inner core and outer core radii χ=r_i/r_o from 0.1 to 0.7 like Heimpel et al. [2005], where r_i and r_o are the inner core radius and the outer core radius, respectively. Long-term variations of the Rayleigh number Ra and the Ekman number E, which are key dimensionless parameters controlling the dynamo action, used in the dynamo simulations are calculated as functions of χ from a thermal history model of the lunar core. Then a relative core evolution curve is drawn, along which we perform a suite of dynamo runs with a given value of χ and with the values of Ra and E that are calibrated by scales of Ra₀=4000, 8000 and 10000, and E₀=O(10^-4). We investigate features of lunar dynamo evolution in scenarios with different values of Ra₀. In summary, we find three types of dynamo regimes during the evolution of lunar core: self-sustaining regime, failing-dynamo regime with convection, and failing-dynamo regime without convection. From the results of the simulations, we find that dynamos cease under a low magnetic Reynolds number that causes the termination of convection because of slow inner core growth in a late phase. We also find that it is difficult to drive convection in the cases of thin shell (χ=0.6 and 0.7) even with the highest Ra₀. This result might suggest a possible scenario in which the lunar dynamo driven by compositional convection shuts off.