Effect of fault bend on the rupture propagation process of stick-slip

被引:27
|
作者
Kato, N
Satoh, T
Lei, XL
Yamamoto, K
Hirasawa, T
机构
[1] Tohoku Univ, Fac Sci, Sendai, Miyagi 9808578, Japan
[2] Geol Survey Japan, Tsukuba, Ibaraki 3058567, Japan
关键词
fault bend; retarded rupture; rock friction; constitutive friction law; earthquake doublet;
D O I
10.1016/S0040-1951(99)00149-3
中图分类号
P3 [地球物理学]; P59 [地球化学];
学科分类号
0708 ; 070902 ;
摘要
An experimental study of stick-slip is performed to examine the effect of a fault bend on the dynamic rupture propagation process, A granite sample used in the experiment has a pre-cut fault that is artificially bent by an angle of 5.6 degrees at the center of the fault along strike, and accordingly the fault consists of two fault segments. The rupture propagation process during stick-slip instability is investigated by analyzing the records of shear strain and relative displacement measured with strain gauge sensors together with the hypocenters of AE (acoustic emission) events detected with piezoelectric transducers. The observed rupture propagation process of typical stick-slip events is as follows. (1) The dynamic rupture started on a fault segment is stopped near the fault bend. (2) The rupture propagation is restarted near the bend on the other fault segment 10.8 ms to 3.5 s after the stop of the first rupture. The delay time of the second rupture decreases with an increase in the slip amount of the first rupture or a decrease in the normal stress acting on the fault segment where the second rupture started. (3) The restarted rupture is not arrested by the presence of a fault bend, and slip occurs over the entire fault. We theoretically analyze the stress concentration near the fault bend to find that the normal stress produced by the preceding slip near the fault bend plays an important part in controlling the rupture propagation. A numerical simulation based on a rate- and state-dependent friction law is performed to interpret physically the retarded rupture in the experiment. The observed time interval of 10.8 ms to 3.5 s between the first rupture and the second is explained by the numerical simulation, suggesting that the rate- and state-dependence of rock friction is a possible mechanism for the retarded rupture on the fault. (C) 1999 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:81 / 99
页数:19
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