2010
DOI: 10.1016/j.epsl.2009.12.051
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Energy consumption by magmatic fragmentation and pyroclast ejection during Vulcanian eruptions

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Cited by 69 publications
(73 citation statements)
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“…Departures from this trend, however, exist if a well-connected pore network efficiently releases pore pressure and reduces the energy available to achieve complete fragmentation (Mueller et al 2005;Mueller 2007). Whilst the process of fragmentation depends on the energy stored in the pore space, the ejection of the fragmented pyroclasts and the progression of an explosive eruption require additional stored energy, transformed into kinetic energy after fragmentation (Alatorre-Ibargüengoitia et al 2010). In other words, the pressure available to drive the ejection of ballistics (P ef ) equals the initial pressure stored in the pore fraction (P 0 ) minus the pressure required to fragment the porous magma (P th ):…”
Section: Fragmentation and Ballistic Ejectionmentioning
confidence: 99%
See 1 more Smart Citation
“…Departures from this trend, however, exist if a well-connected pore network efficiently releases pore pressure and reduces the energy available to achieve complete fragmentation (Mueller et al 2005;Mueller 2007). Whilst the process of fragmentation depends on the energy stored in the pore space, the ejection of the fragmented pyroclasts and the progression of an explosive eruption require additional stored energy, transformed into kinetic energy after fragmentation (Alatorre-Ibargüengoitia et al 2010). In other words, the pressure available to drive the ejection of ballistics (P ef ) equals the initial pressure stored in the pore fraction (P 0 ) minus the pressure required to fragment the porous magma (P th ):…”
Section: Fragmentation and Ballistic Ejectionmentioning
confidence: 99%
“…Colima (red diamond) best fits the criterion of Koyaguchi et al (2008) with S 3 =3.1. In contrast, the average of all volcanic material tends for S 3 =2 MPa (grey line; see Alatorre-Ibargüengoitia et al 2010). The superimposed porosity distribution reveals the material present in the conduit and helps constrain the overpressure required to initiate fragmentation.…”
Section: Eruption-style Transitionmentioning
confidence: 99%
“…The porosity of a rock controls the amount of gas stored and therefore the energy available for release during fragmentation for a given decompression step (Spieler et al, 2004;Alatorre-Ibargüengoitia et al, 2010). Earlier studies have defined the fragmentation threshold (the minimum pore pressure differential required to fully fragment the sample) as being inversely proportional to the porosity (Spieler et al, 2004).…”
Section: Introductionmentioning
confidence: 99%
“…As the purpose of this study is to calculate maximum horizontal ranges of VBPs, an initial pressure of 25 MPa is adopted which implies an overpressure towards the upper end of the range calculated by Burgisser et al (2011). This value is also higher than the initial pressure estimated for Popocatépetl volcano (11-13 MPa) and slightly higher than the one estimated for Colima volcano (19-22 MPa) (Alatorre-Ibargüengoitia et al, 2010).…”
Section: Quantitymentioning
confidence: 89%
“…First, a caprock model proposed by Alatorre-Ibargüengoitia et al (2010) approximating conditions during small volume explosive eruptions is used in order to estimate initial velocities of ejected VBPs. Initial velocities for higher energy eruptions are calculated by using an approach based on the conversion efficiency of thermal to kinetic energy (Sato and Taniguchi, 1997).…”
Section: Introductionmentioning
confidence: 99%