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        <identifier>oai:figshare.com:article/32804315</identifier>
        <datestamp>2026-06-30T11:28:23Z</datestamp>
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          <dc:title>Dynamic Poroelastic Finite Element Deformation Modelling of the Bárðarbunga Volcano, Iceland, 2015-2024</dc:title>
          <dc:creator>Dan Manns (21044948)</dc:creator>
          <dc:subject>Volcanology</dc:subject>
          <dc:subject>Geophysics</dc:subject>
          <dc:subject>Geodesy</dc:subject>
          <dc:subject>Geology</dc:subject>
          <dc:subject>Iceland</dc:subject>
          <dc:subject>Numerical Modelling</dc:subject>
          <dc:subject>Ground Deformation</dc:subject>
          <dc:description>Monitoring and modelling of ground deformation at volcanoes provides key insights into how a subsurface magmatic system is evolving due to magma movements at depth. Here, we present a dynamic poroelastic-reservoir Finite Element (FE) volcano deformation model. This thesis aims to reproduce the observed post-eruptive (2015 – 2024) deformation of the Bárðarbunga volcano to constrain the likely magma supply and storage characteristics. Initial exploratory modelling was undertaken using 2D-axisymmetric FE models to investigate the general effects on surface deformation of poroelastic reservoir geometry, poroelastic parameters, and the inclusion of a caldera ring fault. Exploratory models demonstrated that poroelastic effects influence deformation even at high reservoir melt fractions, and that a sill-shaped geometry and inclusion of a caldera ring fault focus and amplify deformation directly above the magma reservoir. Analytical (inverse) deformation models provided a preliminary range of likely parameters to inform a more complex FE modelling grid search. Following this, a 3D FE volcano deformation model of the Bárðarbunga volcano was constructed, incorporating independent geological, geophysical, and
geochemical data to be as realistic as possible within computational constraints. The model incorporates: a heterogeneous crust informed by a 1D seismic velocity model; real surface topography; a poroelastic magma reservoir informed by past
eruptive deposits; and a caldera ring fault which simulates active slip. Our optimal FE model provides a good statistical fit to the horizontal GNSS data. Optimal model parameters suggest a sill-shaped magma reservoir at 12 km depth, with a melt fraction of 85%, and a volume of accumulated magma of ~0.36 km^3 over a nine-year period, equivalent to an average inflow rate of 1.25 m^3/s. Of the 1.9 km^3
of magma extruded during the previous eruption, our models suggest that ~19% has been resupplied, and, assuming a continued linear melt flux, will take ~47 years to be fully resupplied.&lt;p&gt;&lt;/p&gt;</dc:description>
          <dc:date>2026-06-29T00:00:00Z</dc:date>
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          <dc:type>Thesis</dc:type>
          <dc:identifier>10779/exe.32804315.v1</dc:identifier>
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          <dc:rights>All rights reserved</dc:rights>
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