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Quantitative structural analyses and numerical modelling of ...

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1. <strong>Quantitative</strong> analysis <strong>of</strong> deformation structures <strong>and</strong> their <strong>numerical</strong> <strong>modelling</strong> 9elevation <strong>and</strong> exhumation <strong>of</strong> rocks. The results <strong>of</strong> our model (Fig. 1.3) shows systematicvariability in strain pattern, depending on the convergence angle <strong>and</strong> strain-rate withinthe transpressive zones. This fundamental behaviour could be used to inverse field datainto controlling parameters in both active <strong>and</strong> fossil deformation zone.One <strong>of</strong> the most important published contributions to this topic (Lexa et al., 2003)is based on our detailed <strong>structural</strong> analysis <strong>of</strong> polyphase deformation within the Gemerunit in the Western Carpathians. Here, the Paleozoic rocks deformed during LowerCretaceous convergence form steep cleavage fan between the more rigid blocks <strong>of</strong> eastern<strong>and</strong> western part <strong>of</strong> the Vepor crystalline basement. Moreover, the so-called Trans-Gemeric shear zone is developed along eastern margin <strong>of</strong> the Vepor promontory <strong>and</strong>further east separate Gemer unit into two domains. By contrast, the eastern part <strong>of</strong>the Vepor basement suffered more frontal convergence with Gemer unit documented bydevelopment <strong>of</strong> Eastern Gemer thrust (Fig. 1.4). We tried to justify this complicatedtectonic model using viscous sheet formulation modelled by finite element method, wherewe simulate deformation in front <strong>of</strong> the moving indenter, which progressively deformedviscous domain in between the stationary blocks <strong>of</strong> eastern <strong>and</strong> western Vepor basement<strong>and</strong> which was free to thicken <strong>and</strong> outflow among these blocks.The result <strong>of</strong> <strong>numerical</strong> <strong>modelling</strong> (Fig. 1.5) was more than surprising, since both thesymmetry <strong>and</strong> distribution <strong>of</strong> viscous deformation <strong>of</strong> thin viscous sheet corresponds withsufficient precision to our observations. We consider this model as particularly valuablecontribution to the simulation <strong>of</strong> continental deformation. This example suggests thatthe concept developed since the eighties <strong>of</strong> last century (Engl<strong>and</strong> <strong>and</strong> Houseman, 1986,Houseman <strong>and</strong> Engl<strong>and</strong>, 1986) for deformation lithospheric scale deformations (deformation<strong>of</strong> Tibet in front <strong>of</strong> India indenter) could be successfully applied to significantlysmaller scale <strong>of</strong> geological units.Our simulations showed that our model for transpression was satisfying startingestimate for the deformation evolution in areas with complex kinematic framework. Webelieve that the deformation <strong>of</strong> continental crust is dominantly controlled by the presence<strong>of</strong> lateral inhomogeneities <strong>of</strong> different shape <strong>and</strong> that the deformation is subsequentlypartitioned <strong>and</strong> channelized into narrow zones. Underst<strong>and</strong>ing polyphase deformationas consequence <strong>of</strong> principles <strong>of</strong> continuum mechanics is a challenge that will be testedin the near future theoretically as well as on field examples.Our field studies <strong>and</strong> observations rise the question <strong>of</strong> underst<strong>and</strong>ing the flow kinematicsin anisotropic rocks. The most common kinematic indicators used by field geologistsare “extensional shear b<strong>and</strong>s”, which form basis <strong>of</strong> argumentation in number<strong>of</strong> kinematic orogenic models (e.g. Behrmann, 1988, Neubauer et al., 1999, Platt <strong>and</strong>

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