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dc.contributor.authorAragón, Eugenio
dc.contributor.authorD'Eramo, Fernando J.
dc.contributor.authorPinotti, Lucio P.
dc.contributor.authorDemartis, Manuel
dc.contributor.authorTubía Martínez, José María
dc.contributor.authorWeinberg, Roberto F.
dc.contributor.authorConiglio, Jorge E.
dc.date.accessioned2019-05-13T12:52:18Z
dc.date.available2019-05-13T12:52:18Z
dc.date.issued2019-05
dc.identifier.citationGeoscience Frontiers 10(3) : 1211-1218 (2019)es_ES
dc.identifier.issn1674-9871
dc.identifier.urihttp://hdl.handle.net/10810/32772
dc.description.abstractFinite volumes of magma moving in confinement, store hydraulic potential energy for the generation, control and transmission of power. The Pascal's principle in a hydraulic jack arrangement is used to model the vertical and lateral growth of sills. The small input piston of the hydraulic jack is equivalent to the feeder dike, the upper large expansible piston equivalent to the magmatic chamber and the inertial force of the magma in the dike is the input force. This arrangement is particularly relevant to the case of sills expanding with blunt tips, for which rapid fracture propagation is inhibited. Hydraulic models concur with experimental data that show that lateral expansion of magma into a sill is promoted when the vertical ascent of magma through a feeder dike reaches the bottom contact with an overlying, flat rigid-layer. At this point, the magma is forced to decelerate, triggering a pressure wave through the conduit caused by the continued ascent of magma further down (fluid-hammer effect). This pressure wave can provide overpressure enough to trigger the initial hydraulic lateral expansion of magma into an incipient sill, and still have enough input inertial force left to continue feeding the hydraulic system. The lateral expansion underneath the strong impeding layer, causes an area increase and thus, further hydraulic amplification of the input inertial force on the sides and roof of the incipient sill, triggering further expansion in a self-reinforcing process. Initially, the lateral pressure increase is larger than that in the roof allowing the sill to expand. However, expansion eventually increases the total integrated force on the roof allowing its uplift into either a laccolith, if the roof preserves continuity, or into a piston bounded by a circular set of fractures. Hydraulic models for shallow magmatic chambers, also suggest that laccolith-like intrusions require the existence of a self-supported chamber roof. In contrast, if the roof of magmatic chambers loses the self-supporting capacity, lopoliths and calderas should be expected for more or less dense magmas, respectively, owing to the growing influence of the density contrast between the host rock and the magma. (C) 2018, China University of Geosciences (Beijing) and Peking University. Production and hosting by Elsevier B.V.es_ES
dc.description.sponsorshipWe are particularly indebted to Eduardo Llambias, for his useful advice and stimulating discussions. Ideas and data presented in this manuscript have benefited from an anonymous reviewer. This study is the result of research projects UNLP 11N/689 and 790, CONICET PID 00688: Agencia Nacional PICT 0910/13 and PICT 1754/16. J.M. Tubia thanks the GIU17/033 (UPV/EHU) and CGL2017-82976-P (AEI/FEDER, UE) projects.es_ES
dc.language.isoenges_ES
dc.publisherChina University of Geoscienceses_ES
dc.rightsinfo:eu-repo/semantics/openAccesses_ES
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/es/*
dc.subjectPascal's principlees_ES
dc.subjectgeologic hydraulic jackes_ES
dc.subjectemplacementes_ES
dc.subjectsills growthes_ES
dc.subjectfluid hammeres_ES
dc.subjectHenry mountainses_ES
dc.subjectascentes_ES
dc.subjectsillses_ES
dc.subjectlaccolithses_ES
dc.subjectintrusiones_ES
dc.subjectmechanicses_ES
dc.subjecttransportes_ES
dc.subjectplutonses_ES
dc.subjectrockses_ES
dc.titleResearch PaperMagma chamber growth models in the upper crust: A review of thehydraulic and inertial constraintses_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.rights.holder2018, China University of Geosciences (Beijing) and Peking University. Production and hosting byElsevier B.V. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).es_ES
dc.rights.holderAtribución-NoComercial-SinDerivadas 3.0 España*
dc.relation.publisherversionhttps://www.sciencedirect.com/science/article/pii/S167498711830210X?via%3Dihubes_ES
dc.identifier.doi10.1016/j.gsf.2018.10.005
dc.departamentoesGeodinámicaes_ES
dc.departamentoeuGeodinamikaes_ES


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2018, China University of Geosciences (Beijing) and Peking University. Production and hosting byElsevier B.V. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).
Except where otherwise noted, this item's license is described as 2018, China University of Geosciences (Beijing) and Peking University. Production and hosting byElsevier B.V. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).