日本地球惑星科学連合2023年大会

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[J] 口頭発表

セッション記号 S (固体地球科学) » S-SS 地震学

[S-SS06] 地震発生の物理・断層のレオロジー

2023年5月23日(火) 09:00 〜 10:15 302 (幕張メッセ国際会議場)

コンビーナ:澤井 みち代(千葉大学)、金木 俊也(産業技術総合研究所)、奥脇 亮(筑波大学)、浦田 優美(産業技術総合研究所)、座長:浦田 優美(産業技術総合研究所)、奥脇 亮(筑波大学)


09:00 〜 09:15

[SSS06-01] Dynamic rupture modeling of near-fault co-seismic displacements during the 2022 Taitung earthquake – what can we constrain using near-fault data?

*金子 善宏1Kearse Jesse2,3、脳塚 義豊1、Avouac Jean-Philippe3、Milliner Chris3、Hsu Ya-Ju4 (1.京都大学 理学研究科、2.Victoria University of Wellington、3.California Institute of Technology、4.Academia Sinica)

キーワード:Earthquake source physics、Strong ground motion、Fault friction

Fault friction controls the dynamics of earthquake rupture, yet it is difficult to measure directly in the field. In particular, a slip-weakening distance (Dc) is a key parameter that can be estimated in rare cases when instrumental recordings are made very close to the fault. The 2022 Mw 7.0 Taitung (Taiwan) earthquake occurred in the area of dense instrumentation, with 17 strong-motion stations and 14 high-rate (1 Hz) GNSS receivers surrounding the source area. In particular, 5 strong-motion stations and 6 GNSS receivers are located within the near-fault region (<5 km), and 3 strong-motion sensors are located less than 1 km from the fault rupture. Using strong-motion station F073 located ~200 m from the surface rupture of the main asperity, we estimate Dc in the shallow (<2 km) portion of the fault to be 0.8 m +/- 0.2 m. We also analyze particle motion time histories in a novel way for all the near-fault locations. In addition, we develop dynamic rupture models of the 2022 Taitung earthquake to reproduce the characteristics of near-fault records and infer the fault friction parameters. We find that a model that produces abrupt changes in the rake angle with depth can explain the characteristics of static and dynamic displacements at near-fault sensors on both sides of the fault. Our results also suggest that Dc of 0.7 m in the shallow (<2 km) portion of the fault assumed in our preferred model is consistent with Dc = 0.8 m +/- 0.2 m estimated from the near-fault records. These results suggest that dense near-fault records combined with dynamic rupture simulations can be used to constrain the fault friction parameters.