The failure of frictional interfaces -the process of frictional rupture -is widely assumed to feature crack-like properties, with far-reaching implications for various disciplines, ranging from engineering tribology to earthquake physics. Yet, how the effective crack-like behavior emerges from basic physics and what its range of validity is are not understood. Here we show that for rapid rupture a finite and well-defined stress drop, which is a necessary condition for the existence of a crack-like behavior, is directly related to wave radiation from the frictional interface to the bulks surrounding it (the so-called radiation damping effect) and to long-range bulk elastodynamics, and not exclusively to interfacial physics. Furthermore, we show that the emergence of a stress drop is a finite time effect, mainly limited by the wave travel time in finite systems. The results for rapid rupture are supplemented by predictions for slow rupture. All of the theoretical predictions are supported by available experimental data and by extensive computations. They offer a comprehensive and basic understanding of why, how and to what extent frictional rupture might be viewed as an ordinary fracture process.
I. BACKGROUND AND MOTIVATIONRapid slip along interfaces separating bodies in frictional contact is mediated by the spatiotemporal dynamics of frictional rupture [1,2]. Frictional rupture is a fundamental process of prime importance for a broad range of physical systems, e.g. it is responsible for squealing in car brake pads [3], for bowing on a violin string [4], and for earthquakes along geological faults [5][6][7], to name just a few well-known examples. The essence of frictional rupture propagation is that a state of relatively high slip rate (the rate of interfacial shear displacement discontinuity) behind the rupture edge propagates into a low/vanishing slip rate state ahead of it, cf. Fig. 1. As such, frictional rupture appears to be essentially similar to ordinary tensile (opening) cracks, where a finite tensile displacement discontinuity (broken material) state behind the crack edge propagates into a zero tensile displacement discontinuity (intact material) state ahead of it [8].There is, however, an important fundamental difference between frictional rupture and ordinary tensile cracks that manifests itself in the stress states associated with these two processes. A tensile crack is composed of surfaces that cannot support stress, so the stress behind its edge vanishes. Consequently, tensile crack propagation is a process in which far-field driving stresses that characterize the material state far ahead of the crack edge are eliminated altogether behind it. The stress drop that accompanies tensile crack propagation has dramatic implications. Most notably, the loss of stress bearing capac- * eran.bouchbinder@weizmann.ac.il † jean-francois.molinari@epfl.ch ity along the crack surfaces is compensated by large concentration of deformation and stress near the crack edge, oftentimes in a way that mimics a mathematical s...