日本地球惑星科学連合2023年大会

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セッション記号 S (固体地球科学) » S-CG 固体地球科学複合領域・一般

[S-CG45] Science of slow-to-fast earthquakes

2023年5月25日(木) 10:45 〜 12:15 国際会議室 (IC) (幕張メッセ国際会議場)

コンビーナ:加藤 愛太郎(東京大学地震研究所)、山口 飛鳥(東京大学大気海洋研究所)、濱田 洋平(独立行政法人海洋研究開発機構 高知コア研究所)、Yihe Huang(University of Michigan Ann Arbor)、座長:松澤 孝紀(国立研究開発法人 防災科学技術研究所)、大久保 蔵馬(防災科学技術研究所)

10:45 〜 11:00

[SCG45-16] Dynamic earthquake ruptures and its radiations with off-fault fracture network in various spatial resolutions

*大久保 蔵馬1、Villafuerte Carlos2、Rougier Esteban3、Bhat Harsha S.2 (1.防災科学技術研究所、2.École Normale Supérieure、3.Los Alamos National Laboratory)

キーワード:Off-fault damage、Dynamic rupture modeling、High-frequency radiation、Radiated energy

The high-resolution geological observations show the fracture network in the off-fault medium on a broad length scale, part of which is co-seismically activated during the dynamic earthquake ruptures. The effect of the minimum length scale of off-fault fractures, i.e., the spatial resolution of the off-fault fracture network, on the characteristics of earthquake sources is of great interest to unravel the earthquake source mechanisms. We thus conducted a case study of different sizes of mesh discretization to identify its role in the earthquake source processes.

We modeled a finite planer fault using the combined finite-discrete element method (FDEM). We used the FDEM-based software tool, the hybrid optimization software suite (HOSS) educational version, developed by LANL. In this numerical framework, the minimum length scale of off-fault fractures is determined by the size of the edges of mesh elements. We thus conducted the dynamic earthquake rupture modeling using three different meshes with 1/10, 1/15, and 1/20 of the static process zone size associated with the main fault. Our focus here is not on the common analysis of numerical mesh convergence but on investigating the effect of the length scale of the off-fault fracture network in the rupture dynamics.

The spatial fracture pattern varied due to the topology with different mesh resolutions, while the total seismic moment M0 and the radiated energy ER, which is contributed from both the main fault and the off-fault fractures, were comparable. We then estimated the power spectrum density of the time series of velocity magnitude in the off-fault medium to evaluate the spatial distribution of the radiation field with different frequency ranges. The radiation field associated with the low-frequency range, corresponding to the rupture on the main fault, was similar with different mesh resolutions. We found even the radiation of the middle-frequency range, which involves some contributions from the off-fault fracture network, could be averaged with distance from the damage zone although the location of the localized spot of the peak velocity varies with the pattern of the off-fault fracture network.

Overall, the macroscopic characteristics such as the seismic moment and overall radiated energy can be resolved with standard criteria of mesh size associated with the main fault, while the localized peak of the high-frequency radiation depends on the relations between the mesh-dependent fracture patterns and the location of stations. These analyses will help evaluate the radiation patterns from the earthquake sources with co-seismic off-fault damage in various spatial resolutions.