地震地质 ›› 2025, Vol. 47 ›› Issue (1): 131-149.DOI: 10.3969/j.issn.0253-4967.2025.01.009

• 研究论文 • 上一篇    下一篇

正应力扰动条件下断层泥带黏滑行为、应变场和声发射时空演化特征

余博文(), 马胜利, 张林   

  1. 地震动力学与强震预测全国重点实验室(中国地震局地质研究所), 北京 100029
  • 收稿日期:2024-08-13 修回日期:2025-01-16 出版日期:2025-02-20 发布日期:2025-04-09
  • 作者简介:

    余博文, 男, 1995年生, 现为中国地震局地质研究所固体地球物理学专业在读博士研究生, 从事构造物理学以及诱发地震机理研究, E-mail:

  • 基金资助:
    国家自然科学基金(U1839211); 国家自然科学基金(U2239204)

EFFECTS OF NORMAL STRESS OSCILLATION ON THE STICK-SLIP BEHAVIOR, NEAR-FAULT STRAIN FIELD AND ACOUSTIC EVENTS FOR FAULT GOUGE LAYERS

YU Bo-wen(), MA Sheng-li, ZHANG Lin   

  1. State Key Laboratory of Earthquake Dynamics and Forecasting, Institute of Geology, China Earthquake Administration, Beijing 100029, China
  • Received:2024-08-13 Revised:2025-01-16 Online:2025-02-20 Published:2025-04-09

摘要:

工业注水可引起断层所受应力的扰动, 进而对区域内的地震活动性造成影响。通过实验研究正应力扰动对断层滑动行为的影响有助于理解诱发、触发地震活动机制。文中使用双剪样品结构开展了不同正应力扰动振幅条件下天然断层泥和盐岩断层泥的摩擦实验, 并对断层附近应变场和声发射进行观测。随着正应力扰动振幅增加, 2种断层泥的黏滑应力降增大, 天然断层泥的黏滑时间间隔逐渐增大并趋于离散, 成核位置增多且该阶段无声发射事件。然而盐岩断层泥的黏滑时间间隔几乎不变且始终保持同一位置成核, 其成核时间和和范围随扰动振幅的增加而增大, 声发射事件位置与成核区基本吻合。断面非均匀性和断层泥模量的差异可解释2种断层泥带附近应变场演化的差异。文中研究可为构建考虑应变非均质性和不同断层泥成分的地震成核模型提供实验观测依据。

关键词: 应力扰动, 断层泥, 应变场, 声发射, 摩擦实验

Abstract:

Industrial activities(e.g., natural gas storage and wastewater injection)and certain natural processes(e.g., solid tides and volcanic activity)can induce stress perturbations on faults, potentially influencing seismic activity in affected regions. Understanding how fault systems respond to these stress perturbations is essential for improving the accuracy of seismic event prediction and mitigation strategies. Previous laboratory studies have primarily focused on the impact of stress perturbations on the mechanical properties of fault stick-slip behavior, such as shear stress drop and the timing of periodic stick-slip cycles. Most of these studies have modeled faults using bare rock surfaces. However, obtaining accurate stress measurements on natural faults is challenging due to the limitations of commonly used seismic monitoring technologies, such as GPS, dense seismic arrays, and distributed optical fibers, which are typically deployed on the Earth's surface or in boreholes. This complicates the extrapolation of laboratory findings to field conditions. Moreover, there is a lack of research on the role of fault gouge, which is prevalent in natural fault zones.

This study aims to investigate how stress perturbations influence the physical fields(strain and acoustic emissions)adjacent to a simulated fault containing fault gouge. A double-direct shear sample configuration was employed to replicate the fault, using two types of fault gouge: a natural fault gouge(composed mainly of dolomite, bassanite, calcite, and small amounts of quartz)and pure halite gouge. During quasi-static loading, the natural fault gouge exhibited stick-slip behavior characterized by lower stress drops and self-sustained oscillations during the “stick” phase, while the halite gouge demonstrated regular stick slip with large stress drops. Strain rosettes and acoustic sensors were used to measure shear strain along the gouge layer and detect acoustic emissions(AE)events. In each experiment, a sinusoidal normal stress oscillation with varying amplitudes was applied after several regular stick-slip cycles.

The results indicate that both gouge types exhibited similar mechanical behavior: shear stress drops, fault weakening, and an increase in stick-slip velocity with higher normal stress oscillation amplitudes. However, distinct differences were observed in the strain field response and the distribution of AE events. As the oscillation amplitude increased, the fault with natural fault gouge showed a growing number of nucleation zones, with no AE events occurring during nucleation. Fault rupture eventually became more homogeneous after the stress drop. In contrast, the halite gouge maintained a constant number of nucleation zones, but both the nucleation time and area increased with higher oscillation amplitudes. AE events persisted throughout the nucleation phase, and their locations corresponded closely with the nucleation zones. The fault rupture process remained homogeneous under all conditions for the halite gouge.

Analysis of the normal strain evolution and Young's moduli for the two gouge materials revealed that the natural fault gouge exhibited significantly higher Young's modulus than that of the halite gouge. This suggests that fault heterogeneity and plastic deformation are key factors in the evolution of the strain field. Materials with higher modulus enhance strain field heterogeneity as normal stress oscillation amplitude increases, since asperities in these materials are more responsive to stress variations. In contrast, the softer halite gouge exhibits less sensitivity to stress changes, leading to fewer variations in strain. This mechanism can be well reflected by the spatial-temporal evolution of normal strain for two types of fault gouge layers. This explains why the number of nucleation zones increases with higher oscillation amplitudes in natural gouge but remains unchanged in halite gouge. These findings offer valuable insights for the development of near-surface monitoring programs aimed at assessing seismic activity.

Key words: Stress oscillation, fault gouge, strain field, acoustic events, friction experiment