Deformation, evolution and controls of halokinetic megaflaps driven by vertically-stacked and laterally-shifting depocenters 

dc.contributor.authorFerrer García, J. Oriol (José Oriol)
dc.contributor.authorRoca i Abella, Eduard
dc.contributor.authorRowan, Mark G.
dc.contributor.authorMuñoz, J. A.
dc.contributor.authorGiles, Katherine A.
dc.contributor.authorGratacós Torrà, Òscar
dc.date.accessioned2024-05-22T07:54:27Z
dc.date.available2024-05-22T07:54:27Z
dc.date.issued2024-05-07
dc.date.updated2024-05-22T07:54:32Z
dc.description.abstractMegaflaps comprise steeply dipping to overturned panels of the oldest suprasalt strata flanking steep diapirs, and represent the roofs of early inflated salt. These large-scale structures result from salt-sediment interaction at minibasin scales and entail multiple kilometres of folding and vertical relief. They are divided into two end- member types (halokinetic and contractional) and form by some combination of limb rotation and kink-band migration. They can be difficult to image and interpret adjacent to flaring diapirs and beneath allochthonous salt due to steep bedding dips and suboptimal illumination. Using physical models, we investigate halokinetic megaflaps driven by differential loading. Models with vertically-stacked vs. laterally-shifting loading above a prekinematic layer have been run to determine the main processes and mechanisms controlling the growth and kinematic evolution of megaflaps. Parameters such as the thickness of the prekinematic cover, the width of the proto-salt wall, the synkinematic sedimentation rate, and variations in the mechanical properties of the prekinematic cover have been tested to evaluate their role in megaflap generation. The experimental results demonstrate that in absence of tectonic forces, halokinetic megaflaps are generated by a combination of 1) an early increase of pressure-head gradient between two adjacent minibasins with different rates of sedimentation and subsidence, and 2) the disappearance of this gradient that occurs when welding occurs beneath the more quickly subsiding minibasin. The geometry, kinematic evolution, and degree of small-scale deformation of the megaflaps in our analogue models are consistent with both exposed (e.g., Paradox Basin) and seismically imaged halokinetic megaflaps (e.g., deepwater northern Gulf of Mexico). 
dc.format.extent20 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec748400
dc.identifier.issn0191-8141
dc.identifier.urihttps://hdl.handle.net/2445/211700
dc.language.isoeng
dc.publisherElsevier Ltd
dc.relation.isformatofReproducció del document publicat a: https://doi.org/https://doi.org/10.1016/j.jsg.2024.105149
dc.relation.ispartofJournal of Structural Geology, 2024, vol. 184
dc.relation.urihttps://doi.org/https://doi.org/10.1016/j.jsg.2024.105149
dc.rightscc-by-nc (c) The Authors, 2024
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess
dc.rights.urihttp://creativecommons.org/licenses/by-nc/3.0/es/*
dc.sourceArticles publicats en revistes (Dinàmica de la Terra i l'Oceà)
dc.subject.classificationGeologia estructural
dc.subject.classificationSedimentologia
dc.subject.classificationTectònica salina
dc.subject.otherStructural geology
dc.subject.otherSedimentology
dc.subject.otherTectonique du sel
dc.titleDeformation, evolution and controls of halokinetic megaflaps driven by vertically-stacked and laterally-shifting depocenters 
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/acceptedVersion

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