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The Effects of Weak Dynamic Pulses on the Slip Dynamics of a Laboratory Fault

机译:弱动态脉冲对实验室故障滑动动力学的影响

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Investigated are the regularities of fault slip under weak impulsive disturbances in laboratory experiments. The fault was simulated by an interface between two granite blocks loaded with normal and shear stresses, and the impulsive disturbances were excited by impacts of steel balls. We found that the passage of an elastic wave does not produce any residual displacement in the absence of shear load. But the process of inelastic fault deformation manifests quite vividly even under a slight constant shear stress. The sign of residual deformation does not depend on the direction of pulse propagation, but it does coincide with the direction of the applied shear load. Depending on the stress-strain state of the fault and the parameters of the impact, there are two scenarios of fault evolution: (1) production of residual deformations with decaying amplitudes under repeated cycles or (2) initiation of slow deformation process and accumulation of displacements up to the occurrence of slip instability. In the case of a continuously increased shear load, the effects of weak periodic impacts essentially depend on the initial slip behavior. The weakest effect is observed in the case of high-amplitude stick-slip. In contrast, in the case of slow, irregular quasi-dynamic slip, tapping leads to an almost complete transformation of the potential energy of deformation into aseismic creep. Thus, a short dynamic disturbance propagating within a stressed blocky medium can trigger a slow deformation process whose contribution to the cumulative deformation may be quite appreciable. Because postdynamic movements can contribute substantially, a delay in the manifestation of dynamic events with respect to the moment of the initial disturbance may be observed. In turn, periodic dynamic disturbances of the stress-strain state can essentially change the mode of background seismicity and the proportion of radiation efficiency of events.
机译:研究是实验室实验中弱冲动紊乱下的故障滑动的规律性。故障通过装载正常和剪切应力的两个花岗岩块之间的界面进行模拟,并且通过钢球的影响激发了冲动的障碍。我们发现弹性波的通过在没有剪切载荷的情况下不会产生任何残留位移。但是,即使在轻微的常量剪切应力下,无弹性故障变形的过程也非常生动地显现。残余变形的迹象不依赖于脉冲传播的方向,但它与施加的剪切载荷的方向一致。取决于断层的应力 - 应变状态和影响的参数,有两种故障演化的情况:(1)在重复循环的重复循环下的衰减幅度或(2)开始慢变形过程和积累流离失所达到稳定性的发生。在连续增加的剪切载荷的情况下,弱周期性影响的影响基本上取决于初始滑动行为。在高幅度粘滑的情况下观察到最弱的效果。相比之下,在缓慢,不规则的准动态滑动的情况下,攻丝导致几乎完全地改变变形的潜在能量变为抗震蠕变。因此,在应力块介质内传播的短动态扰动可以触发慢变形过程,其对累积变形的贡献可能非常明显。因为Postynamic运动可以基本上贡献,所以可以观察到相对于初始干扰的瞬间的动态事件的表现延迟。反过来,应力 - 应变状态的周期性动态干扰可以基本上改变背景震荡模式和事件辐射效率的比例。

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