Schematic illustration of fault/fracture reactivation and other risks associated to fluid injection. Sketch focuses on CO2 injection and the potential for inducing fault slip and seismicity. Source: Subsurface Alliance.
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Geology & Geophysics

Your fault stability analysis might be lying to you

The number your geomechanical model spits out looks reassuringly precise. A tau-ratio of 0.76. A critical pore pressure of 55 MPa. A sliding friction coefficient of 0.6. Clean. Definitive. Often misleading

The Mohr space represents stress states and, com­bined with fault strength criteria, is used to assess fault stability. It is simple, elegant, and widely accepted. It is also, when applied deterministically, rather misleading. Mohr circles are built on single best-estimate values for key geomechanical inputs, and they do not reflect the true variability and uncertainty of the subsurface. In other words, the number your model produces may look precise, but that doesn’t make it right.

Your model is not wrong in a way that it would get flagged in a peer re­view. It is wrong because every single one of those inputs has an associat­ed uncertainty. Your friction coef­ficient? Likely taken from literature and assumed to be representative of your fault. Your stress magnitudes? Inferred from leak-off tests and bore­hole breakouts at best from a sparse borehole dataset. Your fault geome­try? Interpreted from limited resolu­tion seismic data… The deterministic model takes all the uncertainties, col­lapses them into a single number, and hands you a verdict: Stick or slip.

Top: Probability distributions of key geomechanical parameters. Left: Mohr space showing in-situ stress state and failure envelope (thick solid lines) for a deterministic scenario, and uncertainty-driven plausible variations (thin grey / blue solid lines). Right: Probability of Tau Ratio ≥ 1.0 (which defines fault instability) for an optimally oriented fault: 12% chance of fault reactivation. Source: Subsurface Alliance.

The final verdict is just one plau­sible scenario, presented without ac­knowledging the many others. And the one place this matters most is fluid injection. In CO₂ storage, wa­ter flooding, wastewater disposal, or geothermal operations, pore pressure increases while reducing the effective stress with every pore volume in­jected, effectively moving the Mohr circle towards failure. The margin between stability and reactivation of­ten lies within the uncertainty range that deterministic models refuse to acknowledge.

The solution is not a complicated fix, yet we often fail to go the extra mile. Instead of treating inputs as fixed val­ues, treat them as distributions: Ranges that, when possible, are quantitatively defined from observed variation across wells in an area. This distinction mat­ters. Field-calibrated uncertainty limits mean the model reflects actual spatial heterogeneity and measurement varia­bility, not generic assumptions. From there, a Monte Carlo simulation runs thousands of realisations, propagating uncertainty in stress magnitudes, pore pressure, and fault properties through the stability calculation. What you get back is not a single number, but a chance of fault slip.

Probabilistic analysis should not be an advanced tool, but due dili­gence. Before committing to the cost and complexity of full 3D numerical models, a Monte Carlo assessment can help depict your risk landscape. If the probability of reactivation is truly zero across the entire input distribution, then results are defendable and it may be all you need. On the other hand, if a chance of fault slip exists, that is your signal to go beyond and commit time and resources to advanced 3D numerical simulations.

The threshold between stopping at the probabilistic assessment or con­tinuing to numerical models is not set in stone; it depends on your risk tol­erance, your regulatory context, and the consequences of getting it wrong. Probabilistic analysis does not make the call for you. It just ensures you are making it with a clear perspective.

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