SHale gas E l ti dExploration and Exploitation induced RisksRisks
Seismic hazard assessment considering fluid-induced seismicity:Seismic hazard assessment considering fluid-induced seismicity:
Inter-event time distribution of seismicity induced by hydraulic fracturing operationsfracturing operations
Alexander Garcia-Aristizabal(AMRA)
Second Annual MeetingBlackpool - June 5-7, 2017
This project has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 640896.
Introduction: IS seismic hazard assessment
Time
SpaceAccurate estimation ofAccurate estimation of
distribution parametersdescribing the statistical
properties (in time) of the Analysis of the Size
p p ( )seismic processes and the eventual relationships with
industrial activity
yspatial
distribution of IS, accounting for
ph sical constraintsAnalysis of the
Propagation
physical constraints (environment and
industrial parameters)
size distribution accounting for
physical constraintspa a e e s)
Integrating detailed subsurface
constraints (environment and
industrial parameters) subsurface
information to reduce the variability
observed in GMPEs
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Characterizing fluid-induced seismicityg yIn time
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Analysis of fluid-induced seismicity Obseervations
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Analysis of fluid-induced seismicity Obseervations
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Analysis of fluid-induced seismicity Obseervations
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Analysis of fluid-induced seismicity Obseervations
- Analysis in the time domainRelations ith ind strial acti it- Relations with industrial activity
- Analysis in the spatial domain
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Proxy case study
Geothermal fieldCooper basin, Australia
High pressure injection into granitic rockThe well (Habanero 1) was completed in granite from 4135 to 4421m and stimulated twice (2003 & 2005)In 2003, over 20000m3 were injectedIn 2005, over 25000m3 were injectedTemperature at the botomhole: ~250°C
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Proxy case study
Geothermal fieldCooper basin, Australia
8 Olympic pools
High pressure injection into granitic rockThe well (Habanero 1) was completed in granite from 4135 to 4421m and stimulated twice (2003 & 2005)In 2003, over 20000m3 were injectedIn 2005, over 25000m3 were injectedTemperature at the botomhole: ~250°C
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Analysis of fluid-induced seismicity
Cooper basin, 2003
FIP → Fracture initiation testLTI L t i j ti t tLTI → Long-term injection test
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Analysis of fluid-induced seismicity
Cooper basin, 2003
FIP-1
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Analysis of fluid-induced seismicity
Cooper basin, 2003
FIP-1
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Analysis of fluid-induced seismicity Cooper basin, 2003
FIP-1 – Injection periodFIP 1 Injection period
During injection periods,
seismicit rateseismicity rateseems to correlatewith injection ratet ject o ate
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Analysis of fluid-induced seismicity Cooper basin, 2003
FIP-1 – 'Free response' periodFIP-1 – Free response period
During the free response periods,seismicity rate decays with timeseismicity rate decays with time
following a decay function7/20
Analysis of fluid-induced seismicity
Summary of models frequently used for analyzing fluid-induced seismicity in the time domain:
The Reasenberg & Jones model (1989, 1990, 1994)
The Epidemic-type aftershock model, ETAS (Hainzl & Ogata 2005)
The Σ-based (seismogenic index) model of Shapiro et al., 2010.
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Analysis of fluid-induced seismicity
Summary of models frequently used for analyzing fluid-induced seismicity in the time domain:
The Reasenberg & Jones model (1989, 1990, 1994)
The Epidemic-type aftershock model, ETAS (Hainzl & Ogata 2005)
The Σ-based (seismogenic index) model of Shapiro et al., 2010.
W i l t 'h b id' (I FR) d li hWe implement a 'hybrid' (I-FR) modeling approach:
Th i j ti /f (I FR) d li h→ The injection/free-response (I-FR) modeling approach
Analysis of injection periods in the time domain
Analysis of free-response periods in the time domainAnalysis of free-response periods in the time domain
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
Analysis of injection periods in the time domain
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
Analysis of injection periods in the time domain
dt
Study of the Distributionh t i i i t t ticharacterizing inter-event times
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
t → inter-event timesDifferent modeling hypotheses:Different modeling hypotheses:
Non-homogeneous Poisson processprocess
Homogeneous Poisson process
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
Modelparameter
determination
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
Modelparameter
determination
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
Modelparameter
determination
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
Modelparameter
determination
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
Modelparameter
determination
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
Exponential(μ parameter)
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
3.2 bbl/min
Exponential(μ parameter)
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
9 bbl/min
Exponential(μ parameter)
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
19 bbl/min
Exponential(μ parameter)
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Analysis of fluid-induced seismicity I-FR approach – Injection periods
Model testing: Forecasting injection-related seismicity (exponential model for Cooper Basin)
Where:
Parameter of the Exponential distribution: Ir_t : Injection rate at
ti twhere:
time t
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Model testing I-FR approach – Injection periods
a) Forecasting injection-related seismicity (from injection rate data)
→ Given (scheduled) injection rates and volumes, can be used to forecast expected seismicity
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Model testing I-FR approach – Injection periods
a) Forecasting injection-related seismicity (from injection rate data)
13/20→ Given (scheduled) injection rates and volumes, can be used to forecast expected seismicity
Model testing I-FR approach – Injection periods
Model testing: Forecasting injection-related seismicityModel testing: Forecasting injection-related seismicity
Model parameters: determined using data fromdetermined using data from
the FIP-1
Target period: FIP-3
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Model testing I-FR approach – Injection periods
Model testing: Forecasting injection-related seismicity
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Model testing I-FR approach – Injection periods
Model testing: Forecasting injection-related seismicityModel testing: Forecasting injection-related seismicity
Model parameters: determined using data fromdetermined using data from
the FIP-1
Target period: Extended injection 1
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Analysis of fluid-induced seismicity I-FR approach – Free response periods
Analysis of free-response periods in the time domain
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Analysis of fluid-induced seismicity I-FR approach – Free response periods
Considering the so-called “trigger models” (Vere-Jones and Davies 1966), it is d th t th b bilit f h k i t ti t ft iassumed that the probability of a shock occurring at a time t after a given
triggering event is proportional to a decay function λ(t).
Regarding the nature of λ(t), different functions can be considered:
An exponential decay,
An inverse power-law decay,
Modified Omori lawModified Omori law,
Etas model,
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Analysis of fluid-induced seismicity I-FR approach – Free response periods
t -> time from the end of injection
→ Modified Omori law,
Free-responseFree response after FIP-1
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Analysis of fluid-induced seismicity I-FR approach – Free response periods
t -> time from the end of injection
→ Modified Omori law,
Free-response Free-response Free-response Free-responseFree response after FIP-1
Free response after FIP-2
Free response after LTI-1
Free response after FIP-3
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Analysis of fluid-induced seismicity I-FR approach – Free response periods
→ Modified Omori law,
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Analysis of fluid-induced seismicity I-FR approach: Analysis in the time domain
Summary
'Free-response'Injection period Free response period
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Analysis of fluid-induced seismicity I-FR approach: Analysis in the time domain
Summary
'Free-response'Injection period Free response period
Rate of eventsRate of events follows a Poisson
processHPP / NHPPHPP / NHPP
Model parameter(s)Model parameter(s)are a function of the fluid injection rate
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Analysis of fluid-induced seismicity I-FR approach: Analysis in the time domain
Summary
'Free-response'Injection period Free response period
Rate of events The rate of events after theRate of events follows a Poisson
processHPP / NHPP
The rate of events after the end of injection modeled using an adequate decay
function λ(t)HPP / NHPP
Model parameter(s) p (and k) of MOL are a f ti f th i j t dModel parameter(s)
are a function of the fluid injection rate
function of the injected volume (or mass)
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Analysis of fluid-induced seismicity I-FR approach: Analysis in the time domain
Summary
'Free-response'Injection period Free response period
HPP / NHPP Decay function λ(t)
Model parameter(s)f ti f th
p (and k) of MOL are a f ti f th i j t dAnalysis in the timeare a function of the
fluid injection ratefunction of the injected
volume (or mass)
Analysis in the time domain
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Forecasting induced seismicity rates
Analysis of fluid-induced seismicity I-FR approach: Analysis in the time domain
Summary I-FR model for Copper Basin
Exponential – Modif. Omori
Seismicity rate:
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Analysis of fluid-induced seismicity I-FR approach: Analysis in the time domain
Summary I-FR model for Copper Basin
Exponential – Modif. Omori
Seismicity rate:
Where:Where:
Parameter of the Exponential distribution:Exponential distribution:
where:
Ir_t : Injection rate attime t
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Analysis of fluid-induced seismicity I-FR approach: Analysis in the time domain
Summary I-FR model for Copper Basin
Exponential – Modif. Omori
Seismicity rate:
Where:Where:
Parameter of the Exponential distribution:Exponential distribution:
where:
Ir_t : Injection rate attime t
Exponent of the difi d O i
V* : Volume Injected( di th FR i d)modified Omori:
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(preceding the FR period)
Analysis of fluid-induced seismicity I-FR approach:
Forecasting seismicity for a full stage (Injection & Free response periods)
Injection Free-responseInjection Free-response
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Back to IS seismic hazard assessment…
Forecasting seismicity Frequency-size distributiong yrates in time and space (Gutenberg-Richter)
Analysis in the time domain
GMPE
IS seismic hazardassessment
Analysis in the spatial domainassessment
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Analysis considering development by multi-stage/well, multi-well/pad, and multi-pad
Next steps
Updating procedure as the site development progresses in time
|
I-FR approach IS Seismic hazard assessment: Output
Next steps
I t ti ith i l PSHA?IS seismic hazard
assessment
Integration with regional PSHA?
Regional context
nt,
epen
dent
depe
nden
ctiv
ity d
e
EGS site Tim
e-d
dust
rial a
cIn
d
Updated hazard assessment (?)( )
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ConclusionsConclusions
Identifying parameters that control seismicity rates is a key element for evaluating the y gseismic hazard of fluid injections
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ConclusionsConclusions
Identifying parameters that control seismicity rates is a key element for evaluating the y gseismic hazard of fluid injections
Si il t th t t i ti it th t ti ti fSimilar to the tectonic activity, the statistics of induced seismicity can be rather well described by relatively simple models well known in statistical seismologystatistical seismology
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ConclusionsConclusionsA modeling framework for describing fluid induced seismicity in time has g g ybeen presented. It is based in two main modeling tools:
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ConclusionsConclusionsA modeling framework for describing fluid induced seismicity in time has g g ybeen presented. It is based in two main modeling tools:
During injection periods:During injection periods:
Seismicity rates are modeled as a (homogeneous or non-homogeneous) Poisson process, whose
t f ti f th t f fl idparameters are a function of the rate of fluid injection.
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ConclusionsConclusionsA modeling framework for describing fluid induced seismicity in time has g g ybeen presented. It is based in two main modeling tools:
During injection periods:During injection periods:
Seismicity rates are modeled as a (homogeneous or non-homogeneous) Poisson process, whose
t f ti f th t f fl idparameters are a function of the rate of fluid injection.
During free response periods (Ir = 0)During free-response periods (Ir = 0),
seismicity rates are modeled using a decay function (e.g., Omori law). The decay rate is mainly
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controlled by the total volume of fluid injected