# Collective properties of injection‐induced earthquake sequences: 1. Model description and directivity bias

- **Authors:** David Dempsey; Jenny Suckale
- **Journal:** Journal of Geophysical Research: Solid Earth, vol. 121(5), pp. 3609-3637 (2016)
- **Publisher:** American Geophysical Union (AGU)
- **DOI (version of record):** [https://doi.org/10.1002/2015jb012550](https://doi.org/10.1002/2015jb012550)
- **This page:** https://ddempsey.github.io/papers/2016-dempsey-collective-properties-injection-induced-earthquake/
- **Open PDF:** [https://ddempsey.github.io/papers/2016-dempsey-collective-properties-injection-induced-earthquake/dempsey2016-collective-properties-injection.pdf](https://ddempsey.github.io/papers/2016-dempsey-collective-properties-injection-induced-earthquake/dempsey2016-collective-properties-injection.pdf) (Accepted manuscript (peer-reviewed, author's version))
- **Full text (Markdown):** [https://ddempsey.github.io/papers/2016-dempsey-collective-properties-injection-induced-earthquake/fulltext.md](https://ddempsey.github.io/papers/2016-dempsey-collective-properties-injection-induced-earthquake/fulltext.md)
- **Notice:** An edited version of this paper was published by AGU. Published 2016 American Geophysical Union. Version of record: https://doi.org/10.1002/2015jb012550
- **Also in:** UC Research Repository, https://hdl.handle.net/10092/105828
- **Explainer:** all explainers on this site are AI-generated.
- **BibTeX:** https://ddempsey.github.io/papers/2016-dempsey-collective-properties-injection-induced-earthquake/citation.bib
- **Topics:** Induced seismicity & faults; Geothermal systems
- **Keywords:** Seismology; Induced seismicity; Geology; Fault (geology); Tectonics; Plume; Geothermal gradient

## In brief

We modelled large catalogues of earthquakes triggered by injecting fluid into a fault. In our model, these ruptures tended to propagate back towards the injection well, where high fluid pressure favours continued rupture. In the strongest case, a sample of three modelled ruptures was enough to detect this bias.

- We coupled a fracture mechanics model of one-dimensional fault rupture with heterogeneous fault stress and simulated fluid pressure around an injection well.
- Modelled tectonic earthquakes mostly ruptured in one direction, equally often either way, with a weaker preference than in 42 observed large shallow earthquakes.
- Injection directly into a fault biased modelled ruptures towards the well, where high fluid pressure lowers the residual strength of the fault.
- The bias was strongest for a pressure front advancing through a stimulated fault and for larger earthquakes, and small when the well was off the fault.
- A statistical test detected the strongest bias in samples of three modelled ruptures, and the weaker bias from radial flow in samples of 20 ruptures above magnitude 2.4.

## The problem

Injecting fluid underground can trigger earthquakes on nearby faults, and
several induced earthquakes in the years before 2016 exceeded magnitude 5.
Raising the fluid pressure inside a fault lowers its frictional strength. The
fault slips once that strength falls to the shear stress, the force per unit
area pushing its two sides past each other. This condition is the
Mohr-Coulomb failure criterion (Hubbert and Rubey, 1959; Raleigh et al.,
1976).

We focused on directivity, which describes whether a rupture
spreads in one direction from its starting point (unilateral) or in both
directions (bilateral). We measured it with the directivity ratio, D, which
takes values from −1 to 1, with 0 for a perfectly bilateral rupture (McGuire
et al., 2002). We gave D a sign relative to the injection well: negative for
ruptures travelling towards it, positive for ruptures travelling away. Our
goal was to determine whether induced earthquakes prefer one direction, and
how many observations it would take to detect that preference.

## What we did

We represented a fault as a line, with shear stress that varies randomly
along it according to a fractal model. An earthquake starts at the point of highest
stress for tectonic loading, or at the first point where rising fluid
pressure has weakened the fault enough. From this hypocentre, two rupture
tips spread in opposite directions. A tip stops when it enters a low-stress
section of fault that cannot supply the energy needed for further
propagation.

We used three alternative scenarios for fluid pressure, the first two from
reservoir simulations. In the first, fluid was injected directly into the
fault and spread outward with constant permeability. In the second, a well
injected into an aquifer. Below the aquifer was impermeable crystalline
basement cut by a permeable fault, similar to wastewater disposal in the
central United States. In the third, pressure was high inside a growing zone
of fault whose permeability had been enhanced by injection, and fell sharply
at its edge. We used this advancing front to approximate stimulation of an
Enhanced Geothermal System.

We compared catalogues of induced earthquakes against a tectonic reference
catalogue of one earthquake on each of 100,000 simulated faults. Magnitudes
were scaled so that rupture of a whole fault gives magnitude 4.5. This value is
within the range of interest for induced seismicity.

## What we found

Ruptures in the tectonic catalogue clustered near D = −1 and D = 1. This agrees with directivity ratios reported for 42 large shallow earthquakes (McGuire et al.,
2002), although the modelled preference is weaker. The distribution is
symmetric about zero. This is because tectonic loading is uniform along the fault.

Hypocentres in the tectonic catalogue cluster near the middle of their
ruptures. However, a hypocentre 40% of the way along a rupture gives D of
about 0.53. For the same rupture, the proportion of unilateral rupture, E,
which changes linearly with hypocentre position, is only 0.2. A small offset of the hypocentre from the
middle therefore gives a large shift towards unilateral rupture.

<div class="widget" id="w-directivity" role="group" aria-label="Interactive diagram of how the position of the hypocentre inside a rupture sets the directivity ratio D and the proportion of unilateral rupture E, using equations 2 and 3 of the paper"></div>

Injection directly into a fault made the distribution asymmetric. More
earthquakes started near the well, and hypocentres tended to be located at
the end of the rupture furthest from the well. Ruptures therefore tended to
propagate back towards the well. The average D of the catalogue, which we
call the directivity bias, became negative. This is
because high fluid pressure lowers the residual strength of the fault, the
strength at which it slides during an earthquake. A rupture inside the
high-pressure zone releases more stress and is more likely to continue
propagating.

The bias was strongest for the advancing front, which raises pressure most
between the hypocentre and the well. It was weaker for radial flow, and
stronger for larger earthquakes. For a well off the fault, the bias was small
and may be too weak to detect.
Because the advancing-front bias depended on injection pressure relative to
how close the fault was to failure, we suggest that a well-constrained bias
gives an approximate measure of that closeness.

We tested detection by comparing random samples from each induced catalogue
with the tectonic distribution, using a Kolmogorov-Smirnov test.
For the advancing front, a sample of three modelled ruptures was enough to
reject the tectonic distribution at 95% confidence. For radial flow, samples of 100 ruptures of
all sizes were not enough. Restricting the sample to earthquakes above
magnitude 2.4 reduced the number needed to 20. We therefore suggest that
efforts to detect the bias focus on larger earthquakes, whose directivity is also
easier to measure. Jonas et al. (2015) analysed three of the larger
earthquakes triggered during the Basel Enhanced Geothermal System
stimulation. These appear to have started at the edge of the stimulated
volume and propagated back towards the well. This behaviour is consistent
with our model.

## Limitations

Our model is one-dimensional. On a real two-dimensional fault, a rupture can
pass around a low-stress barrier that would stop it on a line. We therefore
expect the model to agree qualitatively with real faults, although
quantitative agreement is less likely.

The detection test assumes that tectonic directivity is symmetric. However,
faults with different rock on each side may have a preferred rupture
direction (Ben-Zion, 2001). Uneven loading, or
the ground surface above a dip-slip fault, could also break the symmetry. In
those cases the test could wrongly indicate induced seismicity. Applying it
to dip-slip earthquakes would first require a better description of
directivity in natural dip-slip earthquakes.

## Glossary

An **induced earthquake** is an earthquake triggered by human activity, here
by raising fluid pressure in a fault.

**Shear stress** is the force per unit area acting to slide the two sides of
a fault past each other.

A **fractal model** describes variation that has a similar pattern at every
length scale.

The **hypocentre** is the point where an earthquake rupture starts.

**Directivity** describes whether a rupture spreads from its hypocentre in one
direction (unilateral) or in two (bilateral).

The **directivity ratio**, D, measures directivity on a scale from −1 to 1,
with 0 for a perfectly bilateral rupture.

The **proportion of unilateral rupture**, E, is a second directivity measure
that varies linearly with the position of the hypocentre inside the rupture.

**Directivity bias** is the average directivity ratio of a catalogue, which
is zero when no direction is preferred.

The **Mohr-Coulomb failure criterion** states that a fault slips when the
shear stress on it reaches its frictional strength.

**Residual strength** is the reduced strength of a fault while it slides
during an earthquake.

**Permeability** measures how easily fluid flows through rock.

An **Enhanced Geothermal System** is a geothermal reservoir created by
injecting fluid at high pressure to make hot rock more permeable.

A **Kolmogorov-Smirnov test** checks whether a set of observations could have
come from a given probability distribution.

A **catalogue** is a list of earthquakes with their properties, here modelled.

## Abstract

Induced seismicity is of increasing concern for oil and gas, geothermal, and carbon sequestration operations, with several M &gt; 5 events triggered in recent years. Modeling plays an important role in understanding the causes of this seismicity and in constraining seismic hazard. Here we study the collective properties of induced earthquake sequences and the physics underpinning them. In this first paper of a two‐part series, we focus on the directivity ratio, which quantifies whether fault rupture is dominated by one (unilateral) or two (bilateral) propagating fronts. In a second paper, we focus on the spatiotemporal and magnitude‐frequency distributions of induced seismicity. We develop a model that couples a fracture mechanics description of 1‐D fault rupture with fractal stress heterogeneity and the evolving pore pressure distribution around an injection well that triggers earthquakes. The extent of fault rupture is calculated from the equations of motion for two tips of an expanding crack centered at the earthquake hypocenter. Under tectonic loading conditions, our model exhibits a preference for unilateral rupture and a normal distribution of hypocenter locations, two features that are consistent with seismological observations. On the other hand, catalogs of induced events when injection occurs directly onto a fault exhibit a bias toward ruptures that propagate toward the injection well. This bias is due to relatively favorable conditions for rupture that exist within the high‐pressure plume. The strength of the directivity bias depends on a number of factors including the style of pressure buildup, the proximity of the fault to failure and event magnitude. For injection off a fault that triggers earthquakes, the modeled directivity bias is small and may be too weak for practical detection. For two hypothetical injection scenarios, we estimate the number of earthquake observations required to detect directivity bias.

## Cite

Dempsey, David, Suckale, Jenny (2016). Collective properties of injection‐induced earthquake sequences: 1. Model description and directivity bias. Journal of Geophysical Research: Solid Earth, 121(5), 3609-3637. https://doi.org/10.1002/2015jb012550

```bibtex
@article{dempsey2016collective,
  title = {Collective properties of injection‐induced earthquake sequences: 1. Model description and directivity bias},
  author = {Dempsey, David and Suckale, Jenny},
  journal = {Journal of Geophysical Research: Solid Earth},
  year = {2016},
  volume = {121},
  number = {5},
  pages = {3609-3637},
  publisher = {American Geophysical Union (AGU)},
  doi = {10.1002/2015jb012550},
  url = {https://ddempsey.github.io/papers/2016-dempsey-collective-properties-injection-induced-earthquake/}
}
```