2022
DOI: 10.1130/g50258.1
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Fault surface morphology as an indicator for earthquake nucleation potential

Abstract: Laboratory measurements can determine the potential for geologic materials to generate unstable (seismic) slip, but a direct relation between sliding behavior in the laboratory and physical characteristics observable in the field is lacking, especially for the phyllosilicate-rich gouges that are widely observed in natural faults. We integrated laboratory friction experiments with surface topography microscopy and demonstrated a quantitative correlation between frictional slip behavior and fault surface morphol… Show more

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Cited by 12 publications
(9 citation statements)
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References 43 publications
(17 reference statements)
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“…Most experiments show slip instabilities during the last millimeter of sliding at 10 μm/s (Figure 5). Strain dependence of sliding instabilities is often attributed to microstructural changes with increasing displacement (Scuderi, Marone, et al., 2016; Shreedharan et al., 2019), however previous data using the same device and material show limited changes in microstructure and frictional parameters with increasing slip (Eijsink et al., 2022). Out of all possible combinations of fault‐parallel stiffness k S and normal stiffness k N , there are only two experiments that show stable sliding with no slip events according to our definition; for k S = 14 MPa/mm, and k N = 4.1 and k N = 223 MPa/mm.…”
Section: Resultsmentioning
confidence: 99%
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“…Most experiments show slip instabilities during the last millimeter of sliding at 10 μm/s (Figure 5). Strain dependence of sliding instabilities is often attributed to microstructural changes with increasing displacement (Scuderi, Marone, et al., 2016; Shreedharan et al., 2019), however previous data using the same device and material show limited changes in microstructure and frictional parameters with increasing slip (Eijsink et al., 2022). Out of all possible combinations of fault‐parallel stiffness k S and normal stiffness k N , there are only two experiments that show stable sliding with no slip events according to our definition; for k S = 14 MPa/mm, and k N = 4.1 and k N = 223 MPa/mm.…”
Section: Resultsmentioning
confidence: 99%
“…From our experiments, we use the first sequence of velocity increases (5-8 mm sample displacement) to analyze the velocity-dependent behavior of the material, which in most experiments is complicated in the second sequence (8-11 mm sample displacement) by the occurrence of stick-slip behavior and large stress drops directly after a velocity step (Figure 3A). Frictional behavior can change with displacement, although from a previous study using the same material and type of apparatus, we have shown that the variation in a-b and D c is small after the initial run-in phase (Eijsink et al, 2022). We use the RSFit3000 Matlab script (Skarbek & Savage, 2019) to find the optimal fit for the rate-and-state friction parameters.…”
Section: Discussionmentioning
confidence: 99%
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“…We consider uniform friction properties on the fault, where a = 0.005 and b = 0.004 (a/b = 1.25); these values are within the range (10 −4 to 10 −2 ) obtained in friction experiments on incoming sediments to the Hikurangi margin (e.g., Boulton et al, 2019;Eijsink & Ikari, 2022;. These experiments show that frictional stability trends span rate-strengthening, rate-neutral, and rate-weakening behaviors.…”
Section: Fault Model Parametersmentioning
confidence: 96%