S028-0005
Two timescales of fault stabilization by dilatant hardening: slow slip events followed by prolonged dynamic rupture

Thursday, 10 December 2020
Poster
Taka Kanaya, University of Maryland College Park, College Park, MD, United States and Wenlu Zhu, University of Maryland College Park, Department of Geology, College Park, MD, United States
Abstract:
Triaxial compression experiments were conducted on Fontainebleau sandstone with initial porosities of 4, 6, and 14% at a constant effective pressure of 70 MPa (produced by various combinations of confining and pore pressures) and strain rates of 10-6 to 10-4 /s, along with bulk permeability measurements. Here we report two timescales of fault stabilization by dilatant hardening: long-term stabilization over the entire failure events, and short-term stabilization during the unstable part of failure. (1) 14% porosity samples deformed at all Pc and Pf, and 4-6% porosity samples deformed at low Pc and Pf, show entirely unstable failure. In contrast, 4-6% porosity samples deformed at high Pc and Pf fail slowly over 10-100 seconds, followed by minor unstable failure. The observed stabilization is consistent with that expected from the drainage conditions constrained from bulk permeabilities and far-field strain rates. The timescales of failure observed over a range of strain rates show a unique scaling relationship with the timescale of characteristic strain for a given strain rate: tfailure ~ tdef n. Fully unstable failure shows n ~ 1, while stabilized failure exhibits n ~ 0.07, smaller than n ~ 1/3 predicted from theoretical models of dilatant hardening. (2) In addition, stabilization also occurs during the unstable part of failure. 4-6% porosity samples deformed at high Pc and Pf display prolonged unstable failure (~1 second based on 0.1 MHz strain gage data) along with tremor-like seismicity. In contrast, experiments showing fully unstable failure are marked by distinct, <10 millisecond earthquake-like seismicity. The timescales of prolonged unstable failure show little correlation with imposed strain rates. Thus, our results suggest that, for the long-term stabilization, dilatant hardening is governed by bulk fluid diffusion and far-field strain rate, but, for the short-term stabilization, by much shorter timescales of deformation (e.g., dynamic rupture).