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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 142 (1994), S. 529-543 
    ISSN: 1420-9136
    Keywords: Self-organised criticality ; fractals ; earthquakes ; acoustic emissions ; cellular automata ; dilatancy ; fault valving ; stress corrosion
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract The concept of self-organised criticality (SOC) has recently been suggested as a paradigm for the long-term behaviour of earthquakes, even though many of the currently-proposed models require some tuning of the state variables or local conservation rules to produce the universally-observed Gutenberg-Richter frequency-magnitude distribution witha b value near 1. For example, a systematic negative correlation is predicted between modelb values and the degree of conservation of local force after the slip of a single element in an elastic spring/block/frictional slider model. A similar relation is described here for a cellular automaton model with constitutive laws based on fracture mechanics. Such systems, although critical phenomena in the sense of producing order on all scales, are clearly not universal, and may not in general even be true examples of SOC. Nevertheless they adequately reproduce both the observed power-law (fractal or multifractal) scaling and its reported short-term fluctuation. We also present experimental and field evidence for similar systematic variations inb value with the degree of force conservation (expressed in terms of a normalised crack extension force) during subcritical crack growth involving the physical and chemical influence of pore fluids during a single cycle of failure both in tension and compression. We find that the level of conservation is strongly influenced by fluid-rock interaction under stress, allowing energy partition into processes such as: physico-chemical stress corrosion reactions; the dissolution and precipitation of mineral species on crack surfaces; and the purely mechnical phenomenon of dilatant hardening. All of these are known to occur in the Earth on a local scale, but few have been explicitly included in automaton models of seismicity. The implication is that over long time periods pore fluids may exert a strong physical and chemical influence on the universal state of SOC which the system evolves in a complex interplay of local feedback mechanisms keeping the system near criticality, perhaps most strikingly due to the ‘valve” action of faults. In the short term, crustal fluids might nevertheless be responsible for systematic local fluctuations about this average state.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 133 (1990), S. 283-304 
    ISSN: 1420-9136
    Keywords: Scattering attenuation ; fractal dimension ; subcritical crack growth ; rock fracture
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract Scattering of seismic waves can be shown to have a frequency dependenceQ −1 ∝ ω3−v if scattering is produced by arrays of inhomogeneities with a 3D power spectrumW 3D(k) ∝k −v. In the earth's crust and upper mantle the total attenuation is often dominated by scattering rather than intrinsic absorption, and is found to be frequency dependent according toQ −1 ∝ ωγ, where −1〈γ≤−0.5. IfD 1 is the fractal dimension of the surface of the 3D inhomogeneities measured on a 2D section, then this corresponds respectively to 1.5〈D 1≤1.75, since it can be shown that γ=2(D 1−2). Laboratory results show that such a distribution of inhomogeneities, if due to microcracking, can be produced only at low stress intensities and slow crack velocities controlled by stress corrosion reactions. Thus it is likely that the earth's brittle crust is pervaded by tensile microcracks, at least partially filled by a chemically active fluid, and preferentially aligned parallel to the maximum principal compressive stress. The possibility of stress corrosion implies that microcracks may grow under conditions which are very sensitive to pre-existing heterogeneities in material constants, and hence it may be difficult in practice to separate the relative contribution of crack-induced heterogeneity from more permanent geological heterogeneities. By constrast, shear faults formed by dynamic rupture at critical stress intensities produceD 1=1, consistent with a dynamic rupture criterion for a power law distribution of fault lengths with negative exponentD. The results presented here suggest empirically thatD 1∼-1/2(D+1), thereby providing the basis for a possible framework to unify the interpretation of temporal variations in seismicb-value (b∼-D/2) and the frequency dependence of scattering attenuation (γ).
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 107 (1991), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: Three types of seismic quiescence are recognized in the earthquake cycle. Post-seismic quiescence occurs due to the stress drop caused by a previous major earthquake, and results in long-term seismic gaps; intermediate-term quiescence occurs due to a small stress relxation in the volume around the next mainshock area; and short-term quiescence during foreshock sequences occurs due to slip-weakening or dilatancy hardening concentrated on the nucleation point. In this paper a single quantitative model for intermediate-term and short-term quiescence is developed from (a) observation of subcritical crack growth due to stress corrosion, and (b) a general model for subcritical damage development where a fractal population of fractures results, irrespective of the underlying mechanism. In the former the stress intensity K of a single dominant macrocrack is the appropriate constitutive variable, while the latter more general formulation relies on a mean potential strain energy release rate 〈G〉 proportional to (a) the square of the applied effective stress and (b) the mean fracture length. Stress corrosion provides an important concrete example as well as a useful analogy for interpreting the general theory. We then consider the effect of a stress decrease in the intermediate-term on seismic event rates using the approporiate constitutive laws for both variables. Simple calculations for a material of stress corrosion index n= 30 show that a 45 per cent reduction in event rates is consistent with only a 2 per cent reduction in K, and a 90 per cent reduction results from only a 7 per cent decrease in K. A similar order of magnitude of quiescence can be predicted theoretically by considering the effect of similar small changes in 〈G〉 for a fractal pupulation of faults or cracks averaged over a range of length scales. Such intermediate-term quiescence occurs in the model when K or 〈G〉 decreases because of the reduction in applied stress, during a phase of strain softening late in the earthquake cycle. Such a decrease in K or 〈G〉 moves the system temporarily further from the failure condition K=Kc (or 〈G〉=〈G〉c) and is therefore stable. This temporary stability is consistent with the relatively long duration of intermediate-term quiescence (months or years). Observed intermediate-term seismic quiescences are relatively easily explained in the model by stable, regional decreases in stress in a volume much larger than the mainshock area, but prior to the period when concentrated accelerating crack growth in the nucleation zone dominates the strain softening. The general mechanism is compared to the Kaiser effect as a possible alternative explanation for intermediate-term seismic quiescence. The two models are not necessarily mutually exclusive, though the Kaiser effect involves local stress and strain relaxation, and predicts more abrupt changes in event rate when the stress decreases.Short-term quiescence is also a feature of the general model, and is predicted when a concomitant decrease in seismic b-value occurs, as the larger events near the nucleation zone begin to dominate the stress relaxation, thereby inhibiting fracture on a smaller scale. Thus K (or (C)) are increasing in this phase despite the stress reduction, because the length of the dominant crack (or the mean crack length of the ensemble) is increasing at a rate fast enough to more than offset the stress decrease. This increase in K or (G) means that the system is inherently unstable, consistent with the very short duration (hours or days) of short-term quiescence.
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  • 4
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 115 (1993), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: A modified Griffith criterion for a fractal ensemble of cracks is applied to the interpretation of Acoustic Emission (AE) statistics during the compressional deformation of intact and artificially pre-cut rock specimens in the laboratory. A mean energy release rate per unit crack surface area 〈;G〉 is recovered from the observed AE event rate N and the seismic b value, by calculating an inferred mean crack length and measuring the differential stress s̀ for a range of experimental conditions. Temporal variations in 〈;G〉 under compressive deformation show very similar trends to those predicted by a synoptic model determined by direct extrapolation from observations of subcritical crack growth under tension. (In the tensile case, deformation is centred on a dominant macrocrack and the stress intensity K, which scales as the square root of G, is the relevant measured variable.)The three independent variables measured during the tests (s̀, N, b) are reduced to points that map out a path through a 3-D phase space (〈G〉, N, b), which depends on the material type and the experimental conditions. 2-D slices through this phase space [(〈;G〉, b)] (〈;G〉, b)] are compared with results from the tensile tests [(K, N), (K, b)]. The event rate N is found to scale with √〈;G〉 according to a power law, with an exponent n’ which is smaller than that for tensile fracture, reflecting the greater stability of compressional rock fracture in its early stages. The effective subcritical crack growth index n’ is correlated with the material type and degree of apparent ’ductility’ on a macroscopic scale, with more brittle behaviour corresponding to higher n’. The value of n’ is similar on unloading of the stress after dynamic faulting as on the loading portion, though the curve is systematically offset, most probably due to the material weakening associated with faulting. The model does not apply near the period of dynamic failure, where strong local interactions are dominant. The seismic b value is also found to scale negatively with √〈;G〉, in a manner similar to experiments where K can be measured independently.The acceleration of the mean seismogenic crack length 〈c〉 =f(t) has a similar power-law form to that predicted from Charles’ law for a single tensile macrocrack, with an implied subcritical crack growth index n smaller than that for fracture in compression. The extra dimension introduced by the time dependence of 〈c〉 allows an independent check on the validity of the theory used to calculate 〈;G〉. In particular n’ from the diagram (〈c〉, t) is found to be similar in magnitude to the exponent obtained from the event rate dependence (〈;G〉, N), a phenomenon first discovered by empirical observation of tensile subcritical crack growth.
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  • 5
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 96 (1989), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: A new model is presented which can explain the major temporal fluctuations in seismic b-value in terms of the underlying physical processes of time-varying applied stress and crack growth under conditions of constant strain rate. The model predicts two minima in the b-value, separated by a temporary maximum of inflexion point; a corollary being that a single broad maximum would be expected in scattering attenuation. These fluctuations in b-value are consistent with reported ‘intermediate-term’ and ‘short-term’ earthquake precursors separated by a period of seismic quiescence. We present preliminary results from controlled laboratory experiments and report recent field observations both of which are consistent with the predicted form, and in particular exhibit the distinctive, second short-term anomaly which reaches a value bc= 0.5 during the critical phase.
    Type of Medium: Electronic Resource
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  • 6
    Publication Date: 2012-08-09
    Description: The dilatancy–diffusion hypothesis was one of the first attempts to predict the form of potential geophysical signals that may precede earthquakes, and hence provide a possible physical basis for earthquake prediction. The basic hypothesis has stood up well in the laboratory, where catastrophic failure of intact rocks has been observed to be associated with geophysical signals associated both with dilatancy and pore pressure changes. In contrast, the precursors invoked to determine the predicted earthquake time and event magnitude have not stood up to independent scrutiny. There are several reasons for the lack of simple scaling between the laboratory and the field scales, but key differences are those of scale in time and space and in material boundary conditions, coupled with the sheer complexity and non-linearity of the processes involved. ‘Upscaling’ is recognized as a difficult task in multi-scale complex systems generally and in oil and gas reservoir engineering specifically. It may however provide a clue as to why simple local laws for dilatancy and diffusion do not scale simply to bulk properties at a greater scale, even when the fracture system that controls the mechanical and hydraulic properties of the reservoir rock is itself scale-invariant.
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  • 7
    Publication Date: 1989-01-01
    Print ISSN: 0956-540X
    Electronic ISSN: 1365-246X
    Topics: Geosciences
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  • 8
    Publication Date: 2018-07-02
    Description: Crack damage leading to failure in rocks can be accumulated through cyclic stressing in the crust. However, the vast majority of experimental studies to investigate cyclic stressing apply conventional triaxial stress states (σ1 〉 σ2 = σ3), while in nature the state of stress in the crust is generally truly triaxial (σ1 〉 σ2 〉 σ3). Furthermore, the magnitude of these crustal stresses can vary over time and their orientations can also rotate over time, generating multiple crack populations and bulk anisotropic crack damage. We investigate the evolution of crack damage under both conventional and true triaxial stress conditions by sequentially and cyclically varying stresses in all three principal directions on cubic samples of dry sandstone using independently controlled stress paths. We have measured, simultaneously with stress, the bulk acoustic emission output, as a proxy for crack damage. We report a directionally controlled crack damage memory effect which has implications for the approach to failure in complex tectonic stress environments. ©2018. The Authors.
    Print ISSN: 0094-8276
    Electronic ISSN: 1944-8007
    Topics: Geosciences , Physics
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  • 9
    Publication Date: 2021-09-01
    Print ISSN: 1365-1609
    Electronic ISSN: 1873-4545
    Topics: Architecture, Civil Engineering, Surveying , Geosciences
    Published by Elsevier
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  • 10
    Publication Date: 2004-06-01
    Print ISSN: 0031-9201
    Electronic ISSN: 1872-7395
    Topics: Geosciences , Physics
    Published by Elsevier
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