JpGU-AGU Joint Meeting 2017

講演情報

[JJ] 口頭発表

セッション記号 M (領域外・複数領域) » M-GI 地球科学一般・情報地球科学

[M-GI32] [JJ] 計算科学による惑星形成・進化・環境変動研究の新展開

2017年5月22日(月) 10:45 〜 12:15 104 (国際会議場 1F)

コンビーナ:林 祥介(神戸大学・大学院理学研究科 惑星学専攻/惑星科学研究センター(CPS))、小河 正基(東京大学大学院総合文化研究科広域科学専攻)、井田 茂(東京工業大学大学院理工学研究科地球惑星科学専攻)、草野 完也(名古屋大学宇宙地球環境研究所)、座長:亀山 真典(国立大学法人愛媛大学地球深部ダイナミクス研究センター)

11:15 〜 11:25

[MGI32-09] 粘性率の応力履歴依存性を持つ流体の熱対流によるプレートテクトニクスの3次元シミュレーション

宮腰 剛広1、*小河 正基2亀山 真典3 (1.海洋研究開発機構、2.東京大学、3.愛媛大学)

Rigid tectonic plates separated by sharp plate margins rather steadily move on the Earth. New plate margins develop, only when such tectonic processes as continental collision and vigorous magmatism known as Large Igneous Provinces induce unusually high stress in the lithosphere; once formed, plate margins remain there even after the stress level is reduced to the usual level in the lithosphere. Our earlier two-dimensional numerical studies of thermal convection of a Newtonian temperature-dependent viscosity fluid show that it is crucial to assume a stress-history dependent viscosity to reproduce these features of tectonic plates of the Earth: In our models, the viscosity takes a high value for plate interior, when the stress σ is sufficiently low; the viscosity drops to a low value typical for plate margins, when σ exceeds the rupture strength of plates σp; the viscosity remains low even after σ is reduced below σp, as long as it remains higher than another threshold σm, the coupling strength at plate margins. The viscosity is a two-valued function of stress in the range from σm to σp. We found that the basic features of tectonic plates arise, only when the typical stress in the lithosphere is within this range. We also found that the stress-history dependent viscosity is crucial for reproducing a thermo-chemical pile like the Large Low Shear Velocity Provinces, and to realize the asthenosphere that moves faster than the overlying plates around ridges. In this presentation, we extend this two-dimensional model of mantle convection to three-dimensional space by the use of the ACuTEMAN code we developed earlier. We calculated convection in a rectangular box with σp lower than the typical stress in the lithosphere to start a plate motion, and succeeded in reproducing sharp plate boundaries. We will raise σp and explore how the plates thus started behave, when the stress-history dependent viscosity plays a crucial role in their dynamics.