论文标题
部分可观测时空混沌系统的无模型预测
Fault friction under thermal pressurization during large coseismic-slip Part II: Expansion to the model of frictional slip
论文作者
论文摘要
在Stathas和Stefanou(2022年)中,我们在大量的断层下提出了有界断层孔的摩擦反应。我们通过使用Cosserat微态连续体模型来描述了故障的机械响应的主体滑移区(PSZ)厚度的演变来做到这一点。获得的数值结果与在数学平面上滑动过程中建立的热电联机预测的结果显着不同(参见Mase and Smith(1987); Rice(2006a); Platt等人(2014a)等)。这些差异促使我们重新考虑了原始模型中存在的无界域上固定应变定位的基本假设。我们偏离了这些假设,扩展了模型以结合不同的应变定位模式,温度和孔隙流体压力边界条件。新模型使我们能够对第一部分的详细数值结果进行重大理解。我们研究了分别考虑到有界和无界域的等温线,排水的边界条件,在故障岩石内进行行进应变定位的影响。我们的结果表明,当将固定应变定位曲线应用于有界域时,边界条件会导致稳态,并在达到总强度重新恢复。在行进不稳定的情况下,这种稳定状态是不可能的,并且断层仅恢复其摩擦强度的一部分,具体取决于地震滑速速度和剪切带的行进速度。在这种情况下,还会开发出增加地震频率含量的摩擦振荡。我们的结果表明,重新评估了热加压作为摩擦弱化机制的作用。
In Stathas and Stefanou (2022) we presented the frictional response of a bounded fault gouge under largecoseismic slip. We did so by taking into account the evolution of the Principal Slip Zone (PSZ) thickness using a Cosserat micromorphic continuum model for the description of the fault's mechanical response. The numerical results obtained differ significantly from those predicted by the established model of thermal pressurization during slip on a mathematical plane (see Mase and Smith (1987); Rice (2006a); Platt et al. (2014a) among others). These differences prompt us to reconsider the basic assumptions of a stationary strain localization on an unbounded domain present in the original model. We depart from these assumptions, extending the model to incorporate different strain localization modes, temperature and pore fluid pressure boundary conditions. The new model allows us to gain significant understanding of the detailed numerical results of Part I. We investigate the influence of a traveling strain localization inside the fault gouge considering isothermal, drained boundary conditions for the bounded and unbounded domain respectively. Our results establish that when a stationary strain localization profile is applied on a bounded domain, the boundary conditions lead to a steady state, where total strength regain is achieved. In the case of a traveling instability such a steady state is not possible and the fault only regains part of its frictional strength, depending on the seismic slip velocity and the traveling velocity of the shear band. In this case frictional oscillations increasing the frequency content of the earthquake are also developed. Our results indicate a reappraisal of the role of thermal pressurization as a frictional weakening mechanism.