JpGU-AGU Joint Meeting 2017

講演情報

[EJ] 口頭発表

セッション記号 M (領域外・複数領域) » M-AG 応用地球科学

[M-AG35] [EJ] 海洋地球インフォマティクス

2017年5月20日(土) 13:45 〜 15:15 A01 (東京ベイ幕張ホール)

コンビーナ:坪井 誠司(海洋研究開発機構)、高橋 桂子(国立研究開発法人海洋研究開発機構)、金尾 政紀(国立極地研究所)、Timothy Keith Ahern(Incorporated Research Institutions for Seismology)、座長:坪井 誠司(海洋研究開発機構)、座長:松岡 大祐(海洋研究開発機構 地球情報基盤センター)

15:00 〜 15:15

[MAG35-06] Large Scale Simulations of Dynamic Rupture Propagation to Investigate the Fault Behavior of Mega-Thrust Earthquakes

*津田 健一1宮腰 淳一1Ampuero Jean Paul2今任 嘉幸3杉山 大祐3坪井 誠司3 (1.清水建設 株式会社 技術研究所、2.カリフォルニア工科大 地震学教室、3.海洋研究開発機構)

キーワード:動的断層破壊、スペクトル要素法、地球シミュレータ、すべり弱化距離

The investigation of dynamic rupture propagation is very important to understand the seismic behavior of mega-thrust earthquakes such as the 2011 Tohoku earthquake. The shallow parts of the fault (near the trench) hosted large slip and long period seismic wave radiation, whereas the deep parts of the rupture (near the coast) hosted smaller slip and strong radiation of short period seismic waves. Understanding such depth-dependent feature of the rupture process of the Tohoku earthquake is necessary as it may occur during future mega-thrust earthquakes in this and other regions, such as the Nankai Trough. In order to achieve such understanding, dynamic rupture modeling is an important tool (e.g., Galvez et al., 2014).
In this study, we have simulated the dynamic rupture propagation for models of the Tohoku earthquake. Our large-scale simulations used the 3D spectral element method on unstructured grids (Galvez et al., 2014) with performance tuning for the Earth Simulator at JAMSTEC. The number of elements in the mesh is 4,300,000 with 2 km size and polynomial order 4. The simulation takes around 10 hours of wall-clock time on 512 cores. The effective period for the simulation is longer than 1.2 sec.
Our model reproduced the depth-dependency of the rupture process of the Tohoku earthquake. We also examine the sensitivity of the results to model parameters and assumptions, for instance to the value of the slip weakening distance (Dc). We find that the value of Dc does not affect the final slip distribution, as long as it is small enough to allow the rupture to develop and propagate to the trench. A long Dc (order of 10 m) is reasonable in terms of fracture energy and promotes the generation of long period seismic waves on the shallow part of the fault.