Page 384 - Caldera Volcanism Analysis, Modelling and Response
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Facilitating Dike Intrusions into Ring-Faults                        359


             (contours in Figure 2B) is influenced by the reactivated fault, with larger
             displacement vectors near the fault. The cross-sections show that evacuating the
             magma chamber results in higher horizontal (U x ) and vertical (U z ) displacements
             near the fault. The vertical displacement field U z shows a maximum downward
             displacement centered above the chamber. Similarly, previous researchers have
             discussed the effect of freely slipping faults near magma chambers subject to
             pressure changes (Gargani et al., 2006). Some other studies considered circular
             faults around a magma chamber, as detailed below.


             3.1.3. Deflating spherical magma chamber enclosed by a reactivated ring-
             fault
             A caldera ring-fault can be considered a zone of weakness that may accumulate
             volcano-tectonic strain. In the end-member scenario, caldera ring-faults are free
             to slip, considerably affecting deformation at the surface. Figure 4 shows a circular
             fault at a radius of 10 km circumscribing the deflating magma chamber. The fault
             can be considered a ring-fault peripheral to the active magma system, and can be
             reactivated in dip-slip and strike-slip. All other model parameters are the same as
             described above. The horizontal displacement vectors show material convergence
             towards the reservoir (Figure 4B). In cross-section, the displacement U x shows
             slightly smaller values near the surface (Figure 4C). In contrast, vertical
             displacement U z shows a broad area of subsidence (Figure 4D). The bell-shaped
             area of peak subsidence is less expressed, meaning that subsidence would most likely
             occur as a uniform block, limited by the reactivated ring-fault. There is more
             subsidence than in models lacking such a ring-fault, although the pressure drop
             within the magma chamber is the same (cf. Figure 2). Several previous studies have
             considered the effect of reactivated ring-faults surrounding a magma chamber
             subject to pressure changes, for instance, at the caldera of Campi Flegrei, Italy.
             These studies analyze the extent of deformation due to magmatic or hydrothermal
             activity influenced by fault reactivation (Troise et al., 1997, 2003, 2004; Petrazzuoli
             et al., 1999; Beauducel et al., 2004). It must be noted that the pattern of
             displacement fields can vary depending on the type and geometry of the reactivated
             ring-fault.



             3.2. Predicting the location of ring-dike intrusions

             The following models consider an evacuating magma chamber and a passively
             opening ring-fault. Results are shown in map view and in side views, displaying the
             contoured amount of ring-fault opening. In these calculations, the displacement
             perpendicular to each element of the ring-fault is determined; a positive dis-
             placement means that ring-dike intrusion is facilitated, while a negative
             displacement signifies areas where ring-dike intrusions are hindered. These models
             are designed to predict the most likely location and direction of a ring-dike
             intrusion, based on the assumption that a ring-dike intrusion may preferentially
             occur where the ring-fault is opened.
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