Earthquake source processes are described based on friction laws on faults, bulk constitutive behavior of the surrounding medium, and the stress state of an intricate fault network, including off-fault damage. The combination of these components forms a dynamic earthquake rupture model that accounts for the seismological, geodetic, and geological observations, as well as enables estimation of the earthquake energy budget. While such models help clarify key factors characterizing earthquake source processes, trade-offs among these factors often prevent identifying the dominant physical mechanism. For example, enhanced near-field high-frequency radiation can be attributed to fault roughness, structural heterogeneity, or coseismic off-fault damage (Okubo et al., 2019), each of which can produce similar observational signatures.
To mitigate the modeling uncertainties, information available from laboratory experiments can be utilized, such as fault geometry, bulk elastic properties, stress state, and frictional conditions. Here, I demonstrate this concept through a laboratory study aimed at controlling the size and location of earthquake source patches on a laboratory fault (Okubo et al., in revision). This approach provides a predetermined source configuration that can be incorporated into a dynamic rupture model. Circular gouge patches as earthquake sources were placed on a 4-meter-long laboratory fault in a large-scale biaxial apparatus, generating microearthquakes during the evolution of preslip or afterslip on the entire fault in stick-slip experiments. Acoustic emission waveforms carefully corrected for instrumental response and attenuation suggest that these earthquake clusters exhibit non-self-similar scaling. Using the controlled source geometry and the observed source parameters, we developed a dynamic rupture model that is quantitatively consistent with laboratory observations. Although this model is not a unique solution for explaining the observed non-self-similar scaling, given the limited information available to fully resolve the rupture process even under laboratory conditions, it complements previously proposed models for non-self-similar earthquakes and provides a useful basis for interpreting natural earthquakes.
Close integration of experiments and modeling is key to updating previous findings by addressing limitations in existing modeling frameworks. Large-scale experiments allow for spatially dense measurement arrays relative to the characteristic length scales of dynamic ruptures. Models quantitatively constrained by these high-quality measurements help clarify the details in source processes and play an important role in determining which observables, and at what resolution, are required to effectively monitor faulting activity.