1997
DOI: 10.1007/s000240050028
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Numerical Modelling of Block-structure Dynamics: Application to the Vrancea Region

Abstract: A seismically active region is modelled as a system of absolutely rigid blocks separated by infinitely thin plane faults. The interaction of the blocks along the fault planes and with the underlying medium is viscous-elastic. The system of blocks moves as a consequence of prescribed motion of the boundary blocks and of the underlying medium. When, for some part of a fault plane the stress exceeds a certain strength level, a stress-drop (''a failure'') occurs, and it can cause failures in other parts of the fau… Show more

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Cited by 31 publications
(25 citation statements)
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“…Certainly this implies the availability of data covering the time scale of the tectonic processes, which is not the case for the earthquake catalogues presently available. However, the main trends identified in the reported catalogues could be representative of the potential earthquakes, at least in some cases, as shown by PANZA et al (1997) for the Vrancea seismic region.…”
Section: Introductionmentioning
confidence: 99%
“…Certainly this implies the availability of data covering the time scale of the tectonic processes, which is not the case for the earthquake catalogues presently available. However, the main trends identified in the reported catalogues could be representative of the potential earthquakes, at least in some cases, as shown by PANZA et al (1997) for the Vrancea seismic region.…”
Section: Introductionmentioning
confidence: 99%
“…Panza et al [22] studied a model of block structure dynamics of the Vrancea region where the block system moves due to prescribed horizontal motion of the boundary blocks and of the medium underlying the blocks and showed similar features of real and synthetic catalogues. Here I present a dynamical model of block structure, the principal part of which is a sinking slab (see [2] for more details).…”
Section: Model Of Block-and-fault Dynamicsmentioning
confidence: 94%
“…For all blocks and faults the coefficients in (1) are: K ¼ 1 bar/cm and W ¼ 0.05 cm/bar. For all faults the thresholds for j are: B ¼ 0.1, H f ¼ 0.085, and H s ¼ 0.07, and for W s ¼ 5 cm/bar, like those used in previous studies (i.e., PANZA et al, 1997;SOLOVIEV et al, 2000;VOROBIEVA et al, 2000). These parameters reflect the rheology of fault zones in the dimensionless time domain considered for the modeling; a detailed analysis of these parameters and their relation with published estimations (see, e.g., KARNER et al, 2003) goes beyond the scope of the present study.…”
Section: Numerical Experimentsmentioning
confidence: 99%
“…The output of the modeling consists of kinematical data on the block movements that can be compared with observations (e.g., GPS), as well as of a synthetic earthquake catalog, where each event has origin time, coordinates of epicenter, magnitude and source mechanism. On the basis of the experience accumulated to date, the synthetic earthquake catalog reproduces not only some of the basic global features of observed seismicity like (a) the GutenbergRichter law (e.g., PANZA et al, 1997), (b) the space and time clustering of earthquakes (MAKSIMOV and SOLOVIEV, 1999) and (c) the dependence of the occurrence of large earthquakes on the fragmentation of the faults network, and on the rotation of blocks (KEILIS-BOROK et al, 1997), but also several regional features of seismicity, like (1) the epicenter distribution, (2) the relative level of seismic activity in different areas of the region and (3) the type of fault plane solution.…”
Section: Introductionmentioning
confidence: 99%