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10.1126/science.aag2583 (2016).
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The rate of earthquakes induced by fluid injection from oil
and gas operations in parts of North America has surged in
recent years (1, 2). In many areas, this increase is primarily
associated with high-rate injection of large volumes of
saltwater into porous rock formations (3–5). However, the
U.S., U.K., and Canada each have well documented
earthquakes induced by hydraulic fracturing of low-
permeability shale formations, with reported moment
magnitudes (MW) ranging from 2.0 to 4.6 (6–9). Seismicity
triggered by hydraulic fracturing appears to be strongly
localized. In western Canada, for example, induced
seismicity of MW ≥ 3 is associated with only ~0.3% of
hydraulically fractured wells (2).
While we understand the basic principles of injection-
induced seismicity (10, 11), critical details remain incom-
plete concerning activation of rupture on a fluid-pressurized
fault. For massive saltwater injection into a permeable layer,
we believe the primary triggering mechanism is an increase
in pore pressure within an expanding subsurface volume,
which tends to destabilize pre-existing faults by shifting
stress conditions into the shear-failure regime (1, 10). The
fault-activation process is less clear in the case of hydraulic
fracturing, where injection usually occurs within a highly
impermeable layer, inhibiting diffusive transport of injected
fluids and/or pore pressure (2). Moreover, earthquake nu-
cleation requires unstable slip conditions on a fault, as re-
sistance to sliding must diminish faster than elastic
unloading during fault slip. Yet current rate-and-state con-
stitutive laws for rock friction favor aseismic slip in re-
sponse to increasing pore-fluid pressure (12, 13). Resolving
these apparent inconsistencies and developing valid predic-
tive models for earthquakes induced by hydraulic fracturing
remain important challenges.
Intermittent sequences of induced earthquakes began in
December 2013 within a region of previous seismic quies-
cence west of Fox Creek, Alberta (Fig. 1). These earthquake
sequences exhibit clear spatial and temporal correlation
with hydraulic fracturing of the upper Devonian Duvernay
Formation (9), a prolific hydrocarbon source rock that con-
sists of organic-rich mudstone, interfingered with imperme-
able limestone (14). In response to increased levels of
seismicity, real-time seismographic monitoring in this area
has been enhanced by the installation of a network of
broadband stations (15). In the present study, this network
is supplemented by data from 4 broadband seismograph
stations installed by an oil and gas operator within the most
seismically active part of this region (Fig. 2). The application
of algorithms for template-based matched filtering (16) and
double-difference relocation (17) has yielded improved mag-
nitude detection threshold and better focal-depth resolution
than has heretofore been achieved using regional observa-
tions.
In order to undertake a comprehensive comparison be-
tween seismicity and injection parameters, we compiled
injection data for all wells that were completed in the Du-
vernay zone from December 2014 to March 2015 (18). At six
drilling locations (well pads), hydraulic fracturing was per-
formed in multiple stages within horizontal wellbores. Vir-
tually all of the induced seismicity occurred in spatial
clusters concentrated within a lateral distance of ~2 km
from hydraulically fractured wells (Fig. 2), with sparse de-
tectable earthquake activity in the intervening areas be-
tween clusters. Although no template events were available
with which to detect small earthquakes between clusters,
even without such template events we can confidently ex-
clude inter-cluster seismicity of magnitude greater than MW
2.0 based on the detection characteristics of the local array.
As argued by previous authors on the basis of temporal and
Fault activation by hydraulic fracturing in western Canada
Xuewei Bao and David W. Eaton*
Department of Geoscience, University of Calgary, Calgary, Alberta T1N 1N4, Canada.
*Corresponding author. E-mail: eatond@ucalgary.ca
Hydraulic fracturing has been inferred to trigger the majority of injection-induced earthquakes in western
Canada, in contrast to the midwestern United States where massive saltwater disposal is the dominant
triggering mechanism. A template-based earthquake catalog from a seismically active Canadian shale
play, combined with comprehensive injection data during a 4-month interval, shows that earthquakes are
tightly clustered in space and time near hydraulic fracturing sites. The largest event [moment magnitude
(MW) 3.9] occurred several weeks after injection along a fault that appears to extend from the injection
zone into crystalline basement. Patterns of seismicity indicate that stress changes during operations can
activate fault slip to an offset distance of >1 km, whereas pressurization by hydraulic fracturing into a
fault yields episodic seismicity that can persist for months.
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spatial correlation (2, 9), it is highly unlikely that seismicity
in this area has been primarily induced by saltwater injec-
tion. For example, to the end of the time interval for this
study there was only one saltwater disposal well operating
in this area (Fig. 2), injecting into a layer that is higher in
the stratigraphic succession (Mississippian Debolt For-
mation). After three years of operation to the end of March
2015, the cumulative injected volume at the disposal well
was only 9.94 × 104
m3
, a small volume compared to other
regions where induced seismicity from saltwater disposal
has been documented (19).
For the most part, observed induced seismicity exhibits a
clear temporal correlation with hydraulic-fracturing activi-
ties. As evident from graphs of daily average injection pres-
sure and cumulative injected volume (Fig. 3), most of the
induced seismicity occurred during hydraulic-fracturing
operations at proximal well pads. Cluster 1 is an exception
to this behavior and was seismically active from early Janu-
ary to late March. Persistent but intermittent seismicity
within this cluster lacks any clear indication of Omori-type
decay in seismicity rate, which is generally characteristic of
earthquake aftershock sequences; instead, it is characterized
by three distinct post-treatment event sequences (S1–S3),
each defined by a pattern of increasing/ decreasing event
magnitudes followed by a brief hiatus. The largest induced
earthquake (MW 3.9) took place on 23 January 2015 during
sequence S1, two weeks after completion of hydraulic frac-
turing at pad 1. This event occurred during flowback, a post-
injection process during which fracturing fluid is partially
recovered in a controlled manner (20). This timing invites
speculation that the earthquake was triggered by fluid
withdrawal; however, only ~7% of the injected fluids at well
1 flowed back to the wellhead, an unusually low recovery
level compared to typical values of ~50% in other parts of
western Canada (21). This limited recovery of flowback flu-
ids is indicative of fluid retention within a subsurface region
that is in hydrological contact with the primary or second-
ary network of induced hydraulic fractures (22).
The combined availability of a relatively complete earth-
quake catalog and comprehensive injection data enable accu-
rate determination of several important parameters. For
example, an often-cited relationship postulates that maxi-
mum seismic moment for injection-induced earthquakes is
limited to the product of the net volume of injected fluid and
the effective modulus of rigidity that describes the fault zone
(19). This model assumes that the stimulated rockmass is ful-
ly saturated, proximal faults are critically stressed, brittle
failure occurs within a volume that is weakened by anthropo-
genic pore pressure increase, and induced earthquakes follow
a Gutenberg-Richter magnitude distribution with a b-value
near unity. Based on the cumulative injected volume for each
well pad, we used this relationship to calculate a time-
dependent upper limit for moment magnitude. The calculat-
ed envelope is in general agreement with our observations
(Fig. 3). Similarly, the seismogenic index (Σ), defined as log10
N≥M (t) − log10 VI (t) + b M, provides a measure of site-specific
seismotectonic characteristics that expresses the (time inde-
pendent) potential for induced seismicity per unit injected
fluid volume (23). For a given location, calculation of Σ re-
quires observations of the earthquake magnitude–frequency
distribution, the b parameter of the Gutenberg-Richter scal-
ing law, and the net injected fluid volume, VI. The calculated
seismogenic index for our study area ranges between −2.7
and −1.5. These values of Σ exceed values obtained elsewhere
for hydraulic fracturing (−9.4 to −4.4), but fall within a previ-
ously documented range (23) for geothermal reservoirs (−3.2
to 0.4), suggesting that seismic hazard in the Fox Creek area
may be more typical of that for geothermal projects than for
other shale plays.
An east-west cross section through cluster 1, where the
station geometry is most optimal for determination of pre-
cise focal hypocenter locations, reveals two distinct, steeply
dipping bands of seismicity extending from the injection
zone within the Duvernay Formation into the upper part of
crystalline basement (Fig. 4). These bands of seismicity are
interpreted as en echelon fault strands within a roughly
north-south trending strike-slip fault system, a scenario
consistent with nodal planes evident from regional focal
mechanisms (Fig. 1). Independent support for the existence
of such a fault system is provided by statistical analysis of
seismicity patterns (24), coupled with geochemical models
for widespread dolomitization of the underlying Swan Hills
carbonate platform (25) that invoke basement faults as mi-
gration pathways for large volumes of dolomitizing fluids.
The bulk of seismicity within the east fault strand is located
>1 km from the nearest injection well and, similar to the
other 5 clusters, this strand was mainly active during hy-
draulic-fracturing operations.
In contrast, the more proximal west fault strand was re-
peatedly activated for several months after completion of
the treatment program. The hypocenter distribution sug-
gests that the fault zone intersects the Duvernay Formation
between the two injection wells. Hydraulic fracturing was
performed in these wells using a so-called zipper frac tech-
nique, which involves staggered injection stages between
two wells (26). Considering that ~93% of injected hydraulic
fracturing fluids at well pad 1 were not recovered during
flowback, it is likely that sustained pressurization of the
fault zone occurred. Induced seismicity sequences appear to
have occurred in a retrograde fashion, with the hypocenter
of the largest event (sequence S1) located at the deepest lev-
el within the upper part of Precambrian crystalline base-
ment, followed by migration of subsequent sequences (S2
and S3) to shallower levels, closer to the injection zone.
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A recent analytical study that considered poroelastic
coupling of stress and pore pressure in a homogeneous me-
dium shows that, at large distances from a fluid injection
site, stresses ultimately dominate over pore-pressure in-
crease (27). Similarly, a numerical analysis, also based on
poroelasticity theory, suggests that a 2013–2014 episode of
seismicity induced by hydraulic fracturing in the Fox Creek
area is best explained by the elastic response of the solid
matrix, rather than fluid diffusion (28). In our study, the
east and west strands of cluster 1 appear to delineate faults
with similar orientations but contrasting activation signa-
tures. As shown in fig. S10 of the supplementary materials,
when the elastic response of the surrounding medium to
hydraulic fracturing at well pad 1 is considered, seismicity
within the east strand largely falls within a positive Cou-
lomb stress-change regime (up to ~ 0.1 MPa), consistent
with previous findings (28). On the other hand, hypocenters
for the west strand fall largely within a regime wherein elas-
tic stresses induced by hydraulic fracturing are predicted to
inhibit fault slip, implying that a different triggering mech-
anism is required.
According to a model for nucleation and arrest of dy-
namic rupture on a pressured fault (29), the existence of a
permeable and aerially extensive fault that is imperfectly
aligned with the optimal orientation within the regional
stress field enables pressurization to occur over a large fault
patch prior to nucleation of rupture. As shown in fig. S11 of
the supplementary materials, post-injection activation of the
MW 3.9 earthquake is consistent with pore-pressure diffu-
sion along the west fault strand. Taken together, our obser-
vations suggest that: (i) a ~two-week delay in occurrence of
the largest event after completion of hydraulic fracturing
corresponds with relatively aseismic pressure diffusion on
the west fault strand; (ii) earthquake nucleation occurred
within the uppermost crystalline basement and was trig-
gered by an estimated pore-pressure change of ~ 0.12 MPa;
(iii) the slip regime within the weakened, fluid-pressurized
fault segment above the initial rupture during sequence S1
was subject to re-nucleation during sequences S2 and S3,
months after elastic stresses from the hydraulic fracturing
operations had subsided based on lack of seismicity within
the east fault strand.
The occurrence of the MW 3.9 earthquake on 23 January
2015 prompted, shortly thereafter, the introduction of new
regulations applicable to this region that include a “traffic
light protocol” that mandates immediate shutdown in hy-
draulic fracturing operations following an earthquake of ML
(local magnitude) 4.0 or greater within 5 km of an affected
well (30). Similar magnitude-based traffic-light protocols
have been established in other jurisdictions (31). As seen in
many studies of injection-induced seismicity from massive
saltwater disposal, in this study a reactivated fault zone is
imaged by well-located hypocenters. Our results indicate
that fault activation during and after hydraulic fracturing
can be triggered by different mechanisms, including stress
changes due to the elastic response of the rockmass to hy-
draulic fracturing or pore-pressure changes due to fluid dif-
fusion along a permeable fault zone. While stress-related
triggering appears to diminish shortly after operations, a
fluid-pressurized fault may be susceptible to persistent
seismicity for a period of at least several months. This sug-
gests that increased sensitivity of a fluid-pressurized fault
should be considered in ongoing development of mitigation
strategies for seismicity induced by hydraulic fracturing.
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Acknowledgments
Funding for this study was provided by the Natural Sciences and Engineering
Research Council of Canada (grant IRCSA 485691), Chevron Canada Resources,
Ltd. and the University of Calgary. Telemetered data from the Regional Alberta
Observatory for Earthquake Studies Network (RAVEN) operated by the Alberta
Geological Survey were used in this study. Facilities of IRIS Data Services were
used to access waveforms from the RAVEN network. Seismographic data from
four additional broadband stations, as well as flowback data for well pad 1, were
provided by Repsol Canada. These four stations were installed and operated by
Nanometrics, Ltd. Injection pressures and volumes were accessed under license
from the Well Completions and Frac Database, owned and licensed by Canadian
Discovery Ltd. The injection data can also be accessed online through the
Alberta Energy Regulator at http://aer.ca/, using the well ID numbers listed in
the supplementary material. Generic Mapping Tools (GMT) was used to prepare
several figures. Calculated earthquake magnitudes, hypocenter locations and
injection data are provided as supplementary material. X.B. and D.W.E. both
warrant that they have no conflict of interest in this work.
Supplementary Materials
www.sciencemag.org/cgi/content/full/science.aag2583/DC1
Materials and Methods
Figures S1 to S11
Tables S1 to S7
References (35–47)
31 May 2016; resubmitted 20 June 2016
Accepted 21 October 2016
Published online 17 November 2016
10.1126/science.aag2583
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Fig. 1. Seismicity of northwestern Alberta, Canada for the period
1985−2016. Symbol size indicates magnitude and color denotes date of
occurrence. Seismicity west of Fox Creek commenced in December 2013,
and correlates in space and time with local hydraulic-fracturing operations
(9). Focal mechanisms of the largest earthquakes, from (32–34), are
labeled by year/month/date of occurrence. White rectangle outlines the
area in Fig. 2.
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Fig. 2. Details of seismicity induced by hydraulic fracturing at 6 well
pads from December 2014 to March 2015. Black triangles show local
broadband seismograph stations; small black triangle shows a station that
was deployed for a short time after the MW 3.9 event. Event symbols are
colored by date of occurrence and are scaled based on magnitude. Well
pads are numbered sequentially by initiation of hydraulic-fracturing
operations.
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Fig. 3. Comparison of seismicity and injection schedules for selected
clusters. For each cluster (numbered as in Fig. 2), the upper panel
shows seismicity (red dots) and calculated maximum magnitude (blue
curve) (19), while the lower panel shows average daily treatment
pressure (blue bars) and cumulative injected volume (red curve).
Cluster 1 seismicity is repeated as gray dots in other graphs, for timing
comparison. Black bar graph at top shows number of events per day for
cluster 1, which lacks a typical Omori decay. At well 1, flowback (dashed
curve) indicates recovery of only 7% of injected fluid. S1−S3 indicates
time windows for interpreted sequences. A complete set of graphs for all
clusters is shown in supplementary materials (fig. S9).
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Fig. 4. Cross section through cluster 1, showing east and west fault
strands inferred from double-difference event locations. Dark blue
symbols show events that occurred during hydraulic fracturing in two
horizontal (hz) wells. Light blue, yellow and red symbols show
subsequent events during sequences S1, S2 and S3, respectively.
onNovember21,2016http://science.sciencemag.org/Downloadedfrom
published online November 17, 2016
Xuewei Bao and David W. Eaton (November 17, 2016)
Fault activation by hydraulic fracturing in western Canada
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Study: Fault activation by hydraulic fracturing in western Canada

  • 1. Cite as: X. Bao, D. W. Eaton, Science 10.1126/science.aag2583 (2016). REPORTS First release: 17 November 2016 www.sciencemag.org (Page numbers not final at time of first release) 1 The rate of earthquakes induced by fluid injection from oil and gas operations in parts of North America has surged in recent years (1, 2). In many areas, this increase is primarily associated with high-rate injection of large volumes of saltwater into porous rock formations (3–5). However, the U.S., U.K., and Canada each have well documented earthquakes induced by hydraulic fracturing of low- permeability shale formations, with reported moment magnitudes (MW) ranging from 2.0 to 4.6 (6–9). Seismicity triggered by hydraulic fracturing appears to be strongly localized. In western Canada, for example, induced seismicity of MW ≥ 3 is associated with only ~0.3% of hydraulically fractured wells (2). While we understand the basic principles of injection- induced seismicity (10, 11), critical details remain incom- plete concerning activation of rupture on a fluid-pressurized fault. For massive saltwater injection into a permeable layer, we believe the primary triggering mechanism is an increase in pore pressure within an expanding subsurface volume, which tends to destabilize pre-existing faults by shifting stress conditions into the shear-failure regime (1, 10). The fault-activation process is less clear in the case of hydraulic fracturing, where injection usually occurs within a highly impermeable layer, inhibiting diffusive transport of injected fluids and/or pore pressure (2). Moreover, earthquake nu- cleation requires unstable slip conditions on a fault, as re- sistance to sliding must diminish faster than elastic unloading during fault slip. Yet current rate-and-state con- stitutive laws for rock friction favor aseismic slip in re- sponse to increasing pore-fluid pressure (12, 13). Resolving these apparent inconsistencies and developing valid predic- tive models for earthquakes induced by hydraulic fracturing remain important challenges. Intermittent sequences of induced earthquakes began in December 2013 within a region of previous seismic quies- cence west of Fox Creek, Alberta (Fig. 1). These earthquake sequences exhibit clear spatial and temporal correlation with hydraulic fracturing of the upper Devonian Duvernay Formation (9), a prolific hydrocarbon source rock that con- sists of organic-rich mudstone, interfingered with imperme- able limestone (14). In response to increased levels of seismicity, real-time seismographic monitoring in this area has been enhanced by the installation of a network of broadband stations (15). In the present study, this network is supplemented by data from 4 broadband seismograph stations installed by an oil and gas operator within the most seismically active part of this region (Fig. 2). The application of algorithms for template-based matched filtering (16) and double-difference relocation (17) has yielded improved mag- nitude detection threshold and better focal-depth resolution than has heretofore been achieved using regional observa- tions. In order to undertake a comprehensive comparison be- tween seismicity and injection parameters, we compiled injection data for all wells that were completed in the Du- vernay zone from December 2014 to March 2015 (18). At six drilling locations (well pads), hydraulic fracturing was per- formed in multiple stages within horizontal wellbores. Vir- tually all of the induced seismicity occurred in spatial clusters concentrated within a lateral distance of ~2 km from hydraulically fractured wells (Fig. 2), with sparse de- tectable earthquake activity in the intervening areas be- tween clusters. Although no template events were available with which to detect small earthquakes between clusters, even without such template events we can confidently ex- clude inter-cluster seismicity of magnitude greater than MW 2.0 based on the detection characteristics of the local array. As argued by previous authors on the basis of temporal and Fault activation by hydraulic fracturing in western Canada Xuewei Bao and David W. Eaton* Department of Geoscience, University of Calgary, Calgary, Alberta T1N 1N4, Canada. *Corresponding author. E-mail: eatond@ucalgary.ca Hydraulic fracturing has been inferred to trigger the majority of injection-induced earthquakes in western Canada, in contrast to the midwestern United States where massive saltwater disposal is the dominant triggering mechanism. A template-based earthquake catalog from a seismically active Canadian shale play, combined with comprehensive injection data during a 4-month interval, shows that earthquakes are tightly clustered in space and time near hydraulic fracturing sites. The largest event [moment magnitude (MW) 3.9] occurred several weeks after injection along a fault that appears to extend from the injection zone into crystalline basement. Patterns of seismicity indicate that stress changes during operations can activate fault slip to an offset distance of >1 km, whereas pressurization by hydraulic fracturing into a fault yields episodic seismicity that can persist for months. onNovember21,2016http://science.sciencemag.org/Downloadedfrom
  • 2. First release: 17 November 2016 www.sciencemag.org (Page numbers not final at time of first release) 2 spatial correlation (2, 9), it is highly unlikely that seismicity in this area has been primarily induced by saltwater injec- tion. For example, to the end of the time interval for this study there was only one saltwater disposal well operating in this area (Fig. 2), injecting into a layer that is higher in the stratigraphic succession (Mississippian Debolt For- mation). After three years of operation to the end of March 2015, the cumulative injected volume at the disposal well was only 9.94 × 104 m3 , a small volume compared to other regions where induced seismicity from saltwater disposal has been documented (19). For the most part, observed induced seismicity exhibits a clear temporal correlation with hydraulic-fracturing activi- ties. As evident from graphs of daily average injection pres- sure and cumulative injected volume (Fig. 3), most of the induced seismicity occurred during hydraulic-fracturing operations at proximal well pads. Cluster 1 is an exception to this behavior and was seismically active from early Janu- ary to late March. Persistent but intermittent seismicity within this cluster lacks any clear indication of Omori-type decay in seismicity rate, which is generally characteristic of earthquake aftershock sequences; instead, it is characterized by three distinct post-treatment event sequences (S1–S3), each defined by a pattern of increasing/ decreasing event magnitudes followed by a brief hiatus. The largest induced earthquake (MW 3.9) took place on 23 January 2015 during sequence S1, two weeks after completion of hydraulic frac- turing at pad 1. This event occurred during flowback, a post- injection process during which fracturing fluid is partially recovered in a controlled manner (20). This timing invites speculation that the earthquake was triggered by fluid withdrawal; however, only ~7% of the injected fluids at well 1 flowed back to the wellhead, an unusually low recovery level compared to typical values of ~50% in other parts of western Canada (21). This limited recovery of flowback flu- ids is indicative of fluid retention within a subsurface region that is in hydrological contact with the primary or second- ary network of induced hydraulic fractures (22). The combined availability of a relatively complete earth- quake catalog and comprehensive injection data enable accu- rate determination of several important parameters. For example, an often-cited relationship postulates that maxi- mum seismic moment for injection-induced earthquakes is limited to the product of the net volume of injected fluid and the effective modulus of rigidity that describes the fault zone (19). This model assumes that the stimulated rockmass is ful- ly saturated, proximal faults are critically stressed, brittle failure occurs within a volume that is weakened by anthropo- genic pore pressure increase, and induced earthquakes follow a Gutenberg-Richter magnitude distribution with a b-value near unity. Based on the cumulative injected volume for each well pad, we used this relationship to calculate a time- dependent upper limit for moment magnitude. The calculat- ed envelope is in general agreement with our observations (Fig. 3). Similarly, the seismogenic index (Σ), defined as log10 N≥M (t) − log10 VI (t) + b M, provides a measure of site-specific seismotectonic characteristics that expresses the (time inde- pendent) potential for induced seismicity per unit injected fluid volume (23). For a given location, calculation of Σ re- quires observations of the earthquake magnitude–frequency distribution, the b parameter of the Gutenberg-Richter scal- ing law, and the net injected fluid volume, VI. The calculated seismogenic index for our study area ranges between −2.7 and −1.5. These values of Σ exceed values obtained elsewhere for hydraulic fracturing (−9.4 to −4.4), but fall within a previ- ously documented range (23) for geothermal reservoirs (−3.2 to 0.4), suggesting that seismic hazard in the Fox Creek area may be more typical of that for geothermal projects than for other shale plays. An east-west cross section through cluster 1, where the station geometry is most optimal for determination of pre- cise focal hypocenter locations, reveals two distinct, steeply dipping bands of seismicity extending from the injection zone within the Duvernay Formation into the upper part of crystalline basement (Fig. 4). These bands of seismicity are interpreted as en echelon fault strands within a roughly north-south trending strike-slip fault system, a scenario consistent with nodal planes evident from regional focal mechanisms (Fig. 1). Independent support for the existence of such a fault system is provided by statistical analysis of seismicity patterns (24), coupled with geochemical models for widespread dolomitization of the underlying Swan Hills carbonate platform (25) that invoke basement faults as mi- gration pathways for large volumes of dolomitizing fluids. The bulk of seismicity within the east fault strand is located >1 km from the nearest injection well and, similar to the other 5 clusters, this strand was mainly active during hy- draulic-fracturing operations. In contrast, the more proximal west fault strand was re- peatedly activated for several months after completion of the treatment program. The hypocenter distribution sug- gests that the fault zone intersects the Duvernay Formation between the two injection wells. Hydraulic fracturing was performed in these wells using a so-called zipper frac tech- nique, which involves staggered injection stages between two wells (26). Considering that ~93% of injected hydraulic fracturing fluids at well pad 1 were not recovered during flowback, it is likely that sustained pressurization of the fault zone occurred. Induced seismicity sequences appear to have occurred in a retrograde fashion, with the hypocenter of the largest event (sequence S1) located at the deepest lev- el within the upper part of Precambrian crystalline base- ment, followed by migration of subsequent sequences (S2 and S3) to shallower levels, closer to the injection zone. onNovember21,2016http://science.sciencemag.org/Downloadedfrom
  • 3. First release: 17 November 2016 www.sciencemag.org (Page numbers not final at time of first release) 3 A recent analytical study that considered poroelastic coupling of stress and pore pressure in a homogeneous me- dium shows that, at large distances from a fluid injection site, stresses ultimately dominate over pore-pressure in- crease (27). Similarly, a numerical analysis, also based on poroelasticity theory, suggests that a 2013–2014 episode of seismicity induced by hydraulic fracturing in the Fox Creek area is best explained by the elastic response of the solid matrix, rather than fluid diffusion (28). In our study, the east and west strands of cluster 1 appear to delineate faults with similar orientations but contrasting activation signa- tures. As shown in fig. S10 of the supplementary materials, when the elastic response of the surrounding medium to hydraulic fracturing at well pad 1 is considered, seismicity within the east strand largely falls within a positive Cou- lomb stress-change regime (up to ~ 0.1 MPa), consistent with previous findings (28). On the other hand, hypocenters for the west strand fall largely within a regime wherein elas- tic stresses induced by hydraulic fracturing are predicted to inhibit fault slip, implying that a different triggering mech- anism is required. According to a model for nucleation and arrest of dy- namic rupture on a pressured fault (29), the existence of a permeable and aerially extensive fault that is imperfectly aligned with the optimal orientation within the regional stress field enables pressurization to occur over a large fault patch prior to nucleation of rupture. As shown in fig. S11 of the supplementary materials, post-injection activation of the MW 3.9 earthquake is consistent with pore-pressure diffu- sion along the west fault strand. Taken together, our obser- vations suggest that: (i) a ~two-week delay in occurrence of the largest event after completion of hydraulic fracturing corresponds with relatively aseismic pressure diffusion on the west fault strand; (ii) earthquake nucleation occurred within the uppermost crystalline basement and was trig- gered by an estimated pore-pressure change of ~ 0.12 MPa; (iii) the slip regime within the weakened, fluid-pressurized fault segment above the initial rupture during sequence S1 was subject to re-nucleation during sequences S2 and S3, months after elastic stresses from the hydraulic fracturing operations had subsided based on lack of seismicity within the east fault strand. The occurrence of the MW 3.9 earthquake on 23 January 2015 prompted, shortly thereafter, the introduction of new regulations applicable to this region that include a “traffic light protocol” that mandates immediate shutdown in hy- draulic fracturing operations following an earthquake of ML (local magnitude) 4.0 or greater within 5 km of an affected well (30). Similar magnitude-based traffic-light protocols have been established in other jurisdictions (31). As seen in many studies of injection-induced seismicity from massive saltwater disposal, in this study a reactivated fault zone is imaged by well-located hypocenters. Our results indicate that fault activation during and after hydraulic fracturing can be triggered by different mechanisms, including stress changes due to the elastic response of the rockmass to hy- draulic fracturing or pore-pressure changes due to fluid dif- fusion along a permeable fault zone. While stress-related triggering appears to diminish shortly after operations, a fluid-pressurized fault may be susceptible to persistent seismicity for a period of at least several months. This sug- gests that increased sensitivity of a fluid-pressurized fault should be considered in ongoing development of mitigation strategies for seismicity induced by hydraulic fracturing. References and Notes 1. W. L. Ellsworth, Injection-induced earthquakes. Science 341, 1225942 (2013). doi:10.1126/science.1225942 Medline 2. G. M. Atkinson, D. W. Eaton, H. Ghofrani, D. Walker, B. Cheadle, R. Schultz, R. Shcherbakov, K. Tiampo, J. Gu, R. M. Harrington, Y. Liu, M. van der Baan, H. Kao, Hydraulic fracturing and induced seismicity in the Western Canada Sedimentary Basin. Seismol. Res. Lett. 87, 631–647 (2016). doi:10.1785/0220150263 3. C. Frohlich, Two-year survey comparing earthquake activity and injection-well locations in the Barnett Shale, Texas. Proc. Natl. Acad. Sci. 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Bull. Earthquake Res. Inst. 43, 237–239 (1965). Acknowledgments Funding for this study was provided by the Natural Sciences and Engineering Research Council of Canada (grant IRCSA 485691), Chevron Canada Resources, Ltd. and the University of Calgary. Telemetered data from the Regional Alberta Observatory for Earthquake Studies Network (RAVEN) operated by the Alberta Geological Survey were used in this study. Facilities of IRIS Data Services were used to access waveforms from the RAVEN network. Seismographic data from four additional broadband stations, as well as flowback data for well pad 1, were provided by Repsol Canada. These four stations were installed and operated by Nanometrics, Ltd. Injection pressures and volumes were accessed under license from the Well Completions and Frac Database, owned and licensed by Canadian Discovery Ltd. The injection data can also be accessed online through the Alberta Energy Regulator at http://aer.ca/, using the well ID numbers listed in the supplementary material. Generic Mapping Tools (GMT) was used to prepare several figures. Calculated earthquake magnitudes, hypocenter locations and injection data are provided as supplementary material. X.B. and D.W.E. both warrant that they have no conflict of interest in this work. Supplementary Materials www.sciencemag.org/cgi/content/full/science.aag2583/DC1 Materials and Methods Figures S1 to S11 Tables S1 to S7 References (35–47) 31 May 2016; resubmitted 20 June 2016 Accepted 21 October 2016 Published online 17 November 2016 10.1126/science.aag2583 onNovember21,2016http://science.sciencemag.org/Downloadedfrom
  • 5. First release: 17 November 2016 www.sciencemag.org (Page numbers not final at time of first release) 5 Fig. 1. Seismicity of northwestern Alberta, Canada for the period 1985−2016. Symbol size indicates magnitude and color denotes date of occurrence. Seismicity west of Fox Creek commenced in December 2013, and correlates in space and time with local hydraulic-fracturing operations (9). Focal mechanisms of the largest earthquakes, from (32–34), are labeled by year/month/date of occurrence. White rectangle outlines the area in Fig. 2. onNovember21,2016http://science.sciencemag.org/Downloadedfrom
  • 6. First release: 17 November 2016 www.sciencemag.org (Page numbers not final at time of first release) 6 Fig. 2. Details of seismicity induced by hydraulic fracturing at 6 well pads from December 2014 to March 2015. Black triangles show local broadband seismograph stations; small black triangle shows a station that was deployed for a short time after the MW 3.9 event. Event symbols are colored by date of occurrence and are scaled based on magnitude. Well pads are numbered sequentially by initiation of hydraulic-fracturing operations. onNovember21,2016http://science.sciencemag.org/Downloadedfrom
  • 7. First release: 17 November 2016 www.sciencemag.org (Page numbers not final at time of first release) 7 Fig. 3. Comparison of seismicity and injection schedules for selected clusters. For each cluster (numbered as in Fig. 2), the upper panel shows seismicity (red dots) and calculated maximum magnitude (blue curve) (19), while the lower panel shows average daily treatment pressure (blue bars) and cumulative injected volume (red curve). Cluster 1 seismicity is repeated as gray dots in other graphs, for timing comparison. Black bar graph at top shows number of events per day for cluster 1, which lacks a typical Omori decay. At well 1, flowback (dashed curve) indicates recovery of only 7% of injected fluid. S1−S3 indicates time windows for interpreted sequences. A complete set of graphs for all clusters is shown in supplementary materials (fig. S9). onNovember21,2016http://science.sciencemag.org/Downloadedfrom
  • 8. First release: 17 November 2016 www.sciencemag.org (Page numbers not final at time of first release) 8 Fig. 4. Cross section through cluster 1, showing east and west fault strands inferred from double-difference event locations. Dark blue symbols show events that occurred during hydraulic fracturing in two horizontal (hz) wells. Light blue, yellow and red symbols show subsequent events during sequences S1, S2 and S3, respectively. onNovember21,2016http://science.sciencemag.org/Downloadedfrom
  • 9. published online November 17, 2016 Xuewei Bao and David W. Eaton (November 17, 2016) Fault activation by hydraulic fracturing in western Canada Editor's Summary This copy is for your personal, non-commercial use only. Article Tools http://science.sciencemag.org/content/early/2016/11/16/science.aag2583 tools: Visit the online version of this article to access the personalization and article Permissions http://www.sciencemag.org/about/permissions.dtl Obtain information about reproducing this article: is a registered trademark of AAAS.Scienceall rights reserved. The title Washington, DC 20005. Copyright 2016 by the American Association for the Advancement of Science; December, by the American Association for the Advancement of Science, 1200 New York Avenue NW, (print ISSN 0036-8075; online ISSN 1095-9203) is published weekly, except the last week inScience onNovember21,2016http://science.sciencemag.org/Downloadedfrom