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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 137 (1991), S. 201-219 
    ISSN: 1420-9136
    Keywords: Gas field ; induced seismicity ; rock mechanics ; acoustic emission ; brittle-ductile transition ; sedimentary rocks ; porosity ; triaxial test
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract This study concerns the laboratory testing of core samples from massive sedimentary rocks from an oil and gas field. The depth of extraction of the samples analysed varies between 1000 and 5000 metres. In all, 65 tests were performed, most of which included systematic measurement of acoustic activity during loading. The aim of the testing was to determine which types of fracture could occur in the rock matrix under field-stress conditions by examining in particular the relationship between confining pressure and the transition from brittle to ductile behaviour. The results of the laboratory tests are used to predict the occurrence of seismic activity resulting from the depletion of the gas reservoir which has been monitored during the last twenty years.
    Type of Medium: Electronic Resource
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  • 2
    ISSN: 1420-9136
    Keywords: Induced seismicity ; gas field ; seismic deformation
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract With objective of investigating the peculiarities of seismic process development and seismotectonic deformation character in the focal area of the Gazli earthquakes of 1976 (7.0〈M〈7.3) and 1984 (M=7.2), a local seismic network was installed. For the field observation period (May to June, 1991) more than 400 events with magnitudes −0.2〈M〈4.5 were recorded by at least 6 stations. Isometric presentation of earthquake hypocenters distribution allows us to define the depth and dipping planes orientation of seismoactive faults of the region. The focal mechanisms of 35 earthquakes for the period 1979–1988,M〉2.8, connected to a gas extraction regime period, and 75 events 1〈M〈4.3 for the 1991 period (gas storage regime) are used to analyze the dynamics of seismotectonic deformation processes (SDP) in this region. It has been ascertained, that the earth's crust in the Gazli region is subject to complicated deformation processes, particularly below 4 km depth. The predominant kind of deformation is compression. Vertical velocities of deformation show uplift of most of the region during the period of field work. The maximum velocity of vertical deformations for the Gazli structure isV=0.41 mm/year. The comparison of the vertical velocities' displacements due to seismic flow with recent tectonic movements of the earth's crust has revealed their direct relation and high percentage of seismic flow contribution to the tectonic movement. The results obtained testify that the active seismic processes in the Gazli region are connected not as much as the residual stress release in the focal zone of the earthquakes 05. 1976 and 1984,M〉7.0 but rather with the influence of the gas reservoir exploitational regime on the rocks with different rheologic properties.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 139 (1992), S. 507-534 
    ISSN: 1420-9136
    Keywords: Induced seismicity ; faulting ; fluid ; hydrocarbon ; pore pressure
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract We review earthquake distributions associated with hydrocarbon fields in the context of pore pressure diffusion models, poroelastic stress transfer and isostasy theory. These three mechanisms trigger or induce seismic instabilities at both local scale (D≤5 km) and at regional scale (D≥20 km). The modeled changes in stress are small (≤1 MPa), whatever the tectonic setting. Each mechanism corresponds to different production processes. (1) Local hydraulic fracturing due to fluid injection induces seismic-slip on cracks (M L≤3) within the injected reservoir through decreasing the effective stress. (2) Pure fluid withdrawal causes pore pressure to decrease within the reservoir. It triggers adjustments of the geological structure to perturbations related to the reservoir response to depletion. Poroelastic mechanisms transfer this stress change from the reservoir to the surrounding levels whereM L≤5 seismic instabilities occur either above or below the reservoir. (3) Massive hydrocarbon recovery induces crustal readjustments due to the removal of load from the upper crust. It can induce larger earthquakes (M L≥6) at greater distance from the hydrocarbon fields than the two other mechanisms. Due to the mechanical properties of the shallow rock matrices involved, seismic slip triggered either by mechanism (1) or (2), is a second-order process of the main elastoplastic deformation. for a minimum of 80% of commercially productive basins, most of the local deformation is reported as aseismic, i.e., there is no evidence forM L≥3 earthquakes. Nevertheless, the induced stresses vary as a function of time in a manner that depends on the hydraulic diffusivity (i.e., permeability) of the reservoir and surrounding rocks. Because small earthquakes (M L≤3) indicate changes in stress and pore pressure, monitoring of seismicity is a means of assessingin situ reservoir behavior. The less constrained seismic response to hydrocarbon recovery is the possible connection between local fluid manipulations, triggered earthquakes and major regional earthquakes. Positive feedback mechanisms suggest that the region of seismic hazard changes is much larger than the area where hydrocarbons are extracted. These observations and models testify that fluid movement and pore pressure changes (increase or decrease) play important roles in the mechanics of earthquakes and in the triggering of natural earthquakes.
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  • 4
    ISSN: 1420-9136
    Keywords: Induced seismicity ; faulting ; fluid ; artificial reservoir ; pore pressure ; poroelasticity
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract A sequence of moderate shallow earthquakes (3.5≤M L≤5.3) was located within the Vercors massif (France) in the period 1961–1984. This subalpine massif has been a low seismic area for at least 5 centuries. During the period 1962–1963, 12 shallow earthquakes occurred in the neighborhood (Δ≤10 km) of the Monteynard reservoir, 30 km south of the city of Grenoble. The latest fourM L≥4.0 earthquakes occurred in 1979–1984 either at larger distance (35 km) or greater depth (≥10 km) from the reservoir. Two triggering mechanisms are suggested for this sequence: (i) the direct effect of elastic loading through either increased shear stress or strength reducing by increased pore pressure at depth; (ii) the pore pressure diffusion induced by poroelastic stress change due to the reservoir filling. The weekly water levels, local balanced geological cross sections, and focal mechanisms argue for two types of mechanical connection between the earthquake sequence and the filling cycles of the Monteynard reservoir. The seismic sequence started with the 1962–1963 shallow earthquakes that occurred during the first filling of the reservoir and are typical of the direct effect of elastic loading. The 1979 deeper earthquake is located at a 10 km depth below the reservoir. This event occurred 16 years after the initial reservoir impoundment, but one month after the previous 1963 maximum water level was exceeded. Moreover the yearly reservoir level increased gradually in the period 1962–1979 and has decreased since 1980. Accordingly we suggest that the gradual diffusion of water from reservoir to hypocentral depths decreases the strength of the rock matrices through increased pore pressure. The transition between the two types of seismic response is supported by the analysis ofM L≥3.5 earthquakes which all occurred in the period 1964–1971, ranging between 10 and 30 km distance from the reservoir. The three other delayed earthquakes of the 1961–1984 seismic sequence (M L≥4 during the 1979–1984 period) are all located 35 km away from the reservoir. Based on the seismic activity, the estimates for the hydraulic diffusivities range between 0.2–10 m2/s, except for the first event that occurred 30 km north of the reservoir, the filling just started. The lack ofin situ measurements of crustal hydrological properties in the area, shared by most of the Reservoir-Induced-Seismicity cases, prevents us from obtaining absolute evidence for the triggering processes. These observations and conceptual models attest that previous recurrence times for moderate natural shocks (4.5≤M L≤5.5) estimated within this area using historical data, could be modified by 0.1–1 MPa stress changes. These small changes in deviatoric stress suggest that the upper crust is in this area nearly everywhere at a state of stress near failure. Although the paucity of both number and size of earthquakes in the French subalpine massif shows that aseismic displacements prevail, our study demonstrates that triggered earthquakes are important tools for assessing local seismic risk through mapping fault zones and identifying their possible seismic behavior.
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  • 5
    Publication Date: 2015-10-02
    Description: To understand the complexity and thus to predict earthquake occurrence in size, time, and space, seismicity patterns are characterized by two robust empirical laws: the exponential distribution of magnitude and the power law decrease of aftershock rate over time. These laws are known as the Gutenberg–Richter law and the Omori law, respectively. Using global earthquake catalogs, we resolve that on average the K (aftershock productivity) and the p -value (exponent of the power law decrease of aftershock rate over time) are dependent on the mainshock faulting style. Strike-slip events have a lower aftershock rate ( N ) and K -values and a larger p -value than thrust and normal events, respectively. Within the epidemic-type aftershock sequence model, strong K , N values are driven by a high-branching ratio value ( n ). Within the same framework, a relatively higher n value for the thrust events also predicts the lower p -value we observe for thrust events as compared to strike-slip and normal-faulting events, respectively. Furthermore, we observed that earthquake interactions through time and space are a function of the faulting style when measured by μ ( t ), the exponent of the power law decrease of earthquake density over space. The μ ( t ) values of thrust events for different time windows always remain smaller than those of the strike-slip events. When changes in faulting styles are driven by stress pattern, the Anderson faulting theory predicts thrust faulting that requires somewhat larger stresses, in absolute magnitude, than do normal and strike-slip faulting. Within the framework of rate-and-state friction law, changes in the stress heterogeneity patterns reproduce the p -value changes we observe. Our results suggest that only stress perturbations associated with mainshock rupture affect the productivity and decay rate over time of aftershocks.
    Print ISSN: 0037-1106
    Electronic ISSN: 1943-3573
    Topics: Geosciences , Physics
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  • 6
    Publication Date: 2014-02-04
    Description: The seismicity rate triggered by the Muzaffarabad, Kashmir, 2005 M w  7.6, M s  7.7 earthquake is above the average when analyzing the aftershock rate of the 18 M s ≥7.0 events in the India–Asia collision belt between 1973 and 2008. All 17 M s ≥7.0 events occurred within 10° latitude and 20° longitude distance from the 2005 Muzaffarabad earthquake epicenter. We determined the huge aftershock productivity for this earthquake is not driven by a specific Omori law parameter. This anomaly in aftershock rate value corresponds to a relatively higher rate decay (as measured by the p -value), and a larger density value in a higher background seismicity rate setting (prestress conditions) than the other 17 sequences, respectively. After normalizing by the mainshock size and by the magnitude range of observation, we resolved the anomalies, with a 95% confidence level for five aftershock sequences, for either the duration, the productivity, the density, or the background seismicity rate. When we did not include the local processes that drive these specific anomalies, two other global results emerged for the averaged data from the 18 M s 〉7.0 aftershock sequences. First, for all sequences, background seismicity and duration are anticorrelated ( ). Within the framework of rate-and-state friction law, this result supports the assertion that the observed background seismicity rate can be used as a proxy for the stressing rate ( Dieterich, 1994 ). Second, we robustly resolve the dependence of aftershock productivity on the mainshock faulting styles; for example, the aftershock productivity for strike-slip mainshocks is on average four times smaller than the productivity of thrust faulting mainshocks.
    Print ISSN: 0037-1106
    Electronic ISSN: 1943-3573
    Topics: Geosciences , Physics
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  • 7
    Publication Date: 2018-02-14
    Print ISSN: 0956-540X
    Electronic ISSN: 1365-246X
    Topics: Geosciences
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  • 8
    Publication Date: 2004-07-01
    Print ISSN: 0378-4371
    Electronic ISSN: 1873-2119
    Topics: Physics
    Published by Elsevier
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  • 9
    Publication Date: 2018-09-25
    Description: We analyzed the impact of the 26 largest impounded reservoirs on reservoir‐triggered seismicity (RTS) patterns in the low‐seismicity region of continental France. We treat reservoir‐triggered earthquakes as tectonic earthquakes and apply similar concepts in our analysis. Generally, the spatial extent of an aftershock zone is controlled by the mainshock rupture length. In a similar manner, we use reservoir length as an equivalent length to the rupture length to assess the spatial extent of reservoir‐triggering earthquakes and one to three reservoir lengths as a proxy for the near‐field distance where the stress change induced by reservoir impoundment may trigger seismicity. Accordingly, we define the 1Lr distance as the near‐field reservoir effect on seismicity and the 10Lr distance as the far field, null effect of reservoir stress change on background seismicity. We find that (1) about a quarter of the reservoirs trigger Mmax=2.5–4.7 within the 1Lr distance in a 15 yr space time window, and (2) as tested against a randomized series, superposed epoch analysis demonstrates a robust increase in the average seismicity rate within 2 yrs for the 1–3Lr distance from reservoirs. The reservoirs that trigger in the (1Lr) near‐field distance are significantly larger than the nontriggering ones. While considering the distance of triggering of earthquakes from the reservoir, it is more appropriate to consider the normalized distance (the distance normalized by the reservoir length) to identify earthquake triggering reservoirs at a 1Lr distance. While considering reservoir dimensions, the reservoir length appears to be a more important parameter than the reservoir depth, as the length is proportional to the area of significant stress change. Our results suggest that the RTS mimics the aftershock sequence of a slow reservoir‐impoundment loading, with a corresponding M*reservoir=M(Lr) mainshock magnitude. Further, when considering mainshock–aftershock interactions, our analysis and observations support that the Mmax for RTS for a given reservoir remains, on average, smaller than the reservoir magnitude equivalent.
    Print ISSN: 0037-1106
    Electronic ISSN: 1943-3573
    Topics: Geosciences , Physics
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  • 10
    Publication Date: 2004-02-01
    Print ISSN: 0148-0227
    Electronic ISSN: 2156-2202
    Topics: Geosciences
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