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Structural Development of Calderas                                    291


             3.2. Caldera collapse without regional stress field
             Komuro (1987) is the first attempt to specifically simulate a collapse caldera. This is
             achieved using dry ice evaporating beneath a mixture of sand and clay. The
             spherical dry ice simulates a contracting reservoir extruding magma at surface,
             whereas the sand-clay mixture simulates the upper crust. The length ratio between

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             model and nature is L B10 . As stated by the author, because of the cohesive
             clay, this mixture probably has a strength one order of magnitude larger than
             required to simulate the upper crust. Evaporation of dry ice results in the
             overburden collapse, which propagates upwards to surface, where subcircular ring
             fractures are observed (Figure 2). These are outward dipping in the central part,
             formed at early stages, and subvertical at the periphery of the collapse, formed at
             later stages. The outward dip of the ring faults may permit the intrusion of magma
             during collapse (Figure 2b). No radial fractures are observed.
                Marti et al. (1994) simulate caldera collapse by deflating an elastic balloon
             (magma chamber analogue) within fused alumina powder (upper crust analogue)
             (Figure 3a). Different balloon shapes (spherical, cylindrical, flat, penny-shaped) are
             used to reproduce a wide range of magma chambers. The length ratio between
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             model and nature is L B10 . To simulate collapse, air is removed from the
             balloon. The resulting subsidence is mainly achieved by means of subvertical faults,
             which confine an area characterised by several concentric collapsing blocks; these
             are all bordered by outward dipping reverse faults, each accommodating a minor
             amount of displacement and dying out towards the subvertical faults (Figure 3b).
             Given these concentric ring faults at surface, the authors suggest that nested calderas
             may result from the activity of a single magma chamber. The area of collapse
             increases with the size of the balloon and decreases with its depth.
                Roche et al. (2000) is probably the most detailed and comprehensive
             experimental study focused on collapse calderas so far. Collapses are achieved by
             sinking Newtonian silicone putty (magma analogue) at the base of a sand-pack
             (brittle crust analogue). The sand-silicone interface is flat. Sinking is obtained by





















             Figure 2  Experiments from Komuro (1987). (a) In£ation+de£ation; (b) de£ation only
             (modi¢ed after Komuro,1987).                                                 AU :1
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