Chemical and Biological Physics Department, Weizmann Institute of Science, Rehovot 7610001, Israel.
Department of Physics, The University of Chicago, Chicago, Illinois 60637, USA.
Phys Rev E. 2023 Jan;107(1):L013001. doi: 10.1103/PhysRevE.107.L013001.
A prominent spatiotemporal failure mode of frictional systems is self-healing slip pulses, which are propagating solitonic structures that feature a characteristic length. Here, we numerically derive a family of steady state slip pulse solutions along generic and realistic rate-and-state dependent frictional interfaces, separating large deformable bodies in contact. Such nonlinear interfaces feature a nonmonotonic frictional strength as a function of the slip velocity, with a local minimum. The solutions exhibit a diverging length and strongly inertial propagation velocities, when the driving stress approaches the frictional strength characterizing the local minimum from above, and change their character when it is away from it. An approximate scaling theory quantitatively explains these observations. The derived pulse solutions also exhibit significant spatially-extended dissipation in excess of the edge-localized dissipation (the effective fracture energy) and an unconventional edge singularity. The relevance of our findings for available observations is discussed.
摩擦系统的一种突出的时空失效模式是自修复滑动脉冲,它是一种具有特征长度的传播孤子结构。在这里,我们沿着通用和现实的率态相关摩擦界面数值推导出一族稳态滑动脉冲解,这些界面将接触的大变形体分开。这种非线性界面的摩擦强度作为滑动速度的函数是非单调的,具有局部最小值。当驱动力接近从上方特征局部最小值的摩擦强度时,解表现出发散长度和强烈惯性传播速度,并在远离它时改变其特征。一种近似的标度理论定量解释了这些观察结果。推导出的脉冲解也表现出显著的空间扩展耗散,超过了边缘局部化耗散(有效断裂能)和非常规的边缘奇异。我们的发现对现有观测结果的相关性进行了讨论。