Abstract

Induced seismicity as generated by the injection of fluids in a homogeneous, permeable medium with faults with variable proximity to rupture conditions is simulated using the rate- and state-dependent frictional fault theory (RST) of Dieterich (J Geophys Res 99(B2):2601–2618, 1994) and the critical pressure theory (CPT) developed by Shapiro (Fluid-induced seismicity, Cambridge University Press, Cambridge, 2015). In CPT, the induced local seismicity density is proportional to the pressure rate, limited by the Kaiser Effect, and apparently un-related to the tectonic background seismicity. There is no time delay between a change in pressure rate and seismicity density. As a more complex theory, RST includes a time delay between a pressure change and induced seismicity and it is proportional to the natural tectonic background seismicity. Comparing both modelling approaches at a fixed location, this delay can be significant, dependent on a ‘free’ parameter that represents the lower threshold for pressure below which seismicity is not triggered. This parameter can be tuned so that the results of CPT and RST become similar. Approximations of the RST allow a new interpretation of the parameter ‘tectonic potential’ that controls the level of induced seismicity in CPT.

Highlights

  • Gaucher et al (2015) provide an overview on published methods employed for modelling induced seismicity in geothermal reservoirs

  • In critical pressure theory (CPT), the induced local seismicity density is proportional to the pressure rate, limited by the Kaiser Effect, and apparently un-related to the tectonic background seismicity

  • This leads to a model where the seismicity density at a site is proportional to the temporal pressure derivative at this site

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Summary

Background

Gaucher et al (2015) provide an overview on published methods employed for modelling induced seismicity in geothermal reservoirs. The section represents a summary of the essentials of the critical pressure theory (CPT) including the Kaiser Effect and the rate- and state-dependent theory (RST), which was originally set up for sudden change of shear stress (earthquakes) and has been modified for the case of pressure changes by Wenzel (2015). The seismicity emerges from the space-dependent fault density nf x by integration over space (d3x → dV ) It represents the number of events per unit time with magnitudes above zero for the entire volume that is affected by the pressure diffusion. As Dieterich (1994) studied a step-wise change of shear stress in the neighbourhood of a ruptured fault that generates aftershocks, it is interesting to see how induced seismicity emerges in response to a sudden change in pressure.

50 MPa and
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