Conditions for the occurrence of seismic sequences in a fault system

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Abstract

We consider a fault system producing a sequence of seismic events of similar magnitudes. If the system is made up of n faults, there are n! possible sequences, differing from each other for the order of fault activation. Therefore the order of events in a sequence can be expressed as a permutation of the first n integers. We investigate the conditions for the occurrence of a seismic sequence and how the order of events is related to the initial stress state of the fault system. To this aim, we consider n coplanar faults placed in an elastic half-space and subject to a constant and uniform strain rate by tectonic motions. We describe the state of the system by n variables that are the Coulomb stresses of the faults. If we order the faults according to the magnitude of their Coulomb stresses, a permutation of the first n integers can be associated with each state of the system. This permutation changes whenever a fault produces a seismic event, so that the evolution of the system can be described as a sequence of permutations. A crucial role is played by the differences between Coulomb stresses of the faults. The order of events implicit in the initial state is modified due to changes in the differences between Coulomb stresses and to different stress drops of the events. We find that the order of events is determined by the initial stress state, the stress drops and the stress transfers associated with each event. Therefore the model allows the retrieval of the stress states of a fault system from the observation of the order of fault activation in a seismic sequence. As an example, the model is applied to the 2012 Emilia (Italy) seismic sequence and enlightens the complex interplay between the fault dislocations that produced the observed order of events.

Figures

  • Figure 1. Sketch of the model with n coplanar faults. The x axis is the strike direction. Distances rij between the ith and j th faults are computed from the fault centres.
  • Figure 2. Evolution of a system made up of three faults (n= 3), represented in the state space: (a) the hexagon H , defined in Sect. 7, with its subsets labelled by the associated permutations; (b) states of the system during a seismic sequence: P0 is the initial state; Pi (i = 1,2,3) is the state after the ith event of th seq e ce; (c) magnification of H sh wing the initial and final st t s P0 and P3.
  • Figure 5. Seismic moments mi of the events in the 2012 Emilia sequence. The upper scale indicates the fault number, the lower scale the order of activation. The two strings of numbers yield the permutation α∗ in Eq. (62).
  • Figure 3. Evolution of a system made up of three faults (n= 3): components of the state vector x as functions of time during the seismic sequence shown in Fig. 2 (τ = 1 MPa, δt = 1 a). The steps labelled by i = 1, 2 and 3 correspond to the occurrence of the events in the sequence.
  • Figure 4. Geographic location of the 2012 Emilia seismic sequence (Italy). Stars indicate the epicentres; numbers indicate the order of fault activation.
  • Figure 7. Components of the state vector x at the beginning (a) and at the end (b) of the 2012 Emilia seismic sequence, as calculated from the model. Faults are numbered from west to east. The mean x̄ and the standard deviation s are shown.
  • Table 1. Data for the seismic events of the 2012 Emilia sequence. The origin times and the seismic moments mi are taken from Pezzo et al. (2013) and Tramelli et al. (2014), respectively. The areas Ai take into account the analysis of Caporali and Ostini (2012) and Serpelloni et al. (2012). Fault slips ui are calculated from mi and Ai . See Fig. 6 for fault numbers.

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APA

Dragoni, M., & Lorenzano, E. (2016). Conditions for the occurrence of seismic sequences in a fault system. Nonlinear Processes in Geophysics, 23(6), 419–433. https://doi.org/10.5194/npg-23-419-2016

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