Michelle Parks
University of Iceland
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Featured researches published by Michelle Parks.
Science | 2016
Magnús T. Gudmundsson; Kristín Jónsdóttir; Andrew Hooper; Eoghan P. Holohan; Sæmundur A. Halldórsson; Benedikt Ofeigsson; Simone Cesca; Kristin S. Vogfjord; Freysteinn Sigmundsson; Thórdís Högnadóttir; Páll Einarsson; Olgeir Sigmarsson; A. H. Jarosch; Kristján Jónasson; Eyjólfur Magnússon; Sigrún Hreinsdóttir; Marco Bagnardi; Michelle Parks; Vala Hjörleifsdóttir; Finnur Pálsson; Thomas R. Walter; Martin P.J. Schöpfer; Sebastian Heimann; Hannah I. Reynolds; Stéphanie Dumont; E. Bali; Gudmundur H. Gudfinnsson; Torsten Dahm; Matthew J. Roberts; Martin Hensch
Driven to collapse Volcanic eruptions occur frequently, but only rarely are they large enough to cause the top of the mountain to collapse and form a caldera. Gudmundsson et al. used a variety of geophysical tools to monitor the caldera formation that accompanied the 2014 Bárdarbunga volcanic eruption in Iceland. The volcanic edifice became unstable as magma from beneath Bárdarbunga spilled out into the nearby Holuhraun lava field. The timing of the gradual collapse revealed that it is the eruption that drives caldera formation and not the other way around. Science, this issue p. 262 Magma flow from under the Bárdarbunga volcano drove caldera collapse during the 2014 eruption. INTRODUCTION The Bárdarbunga caldera volcano in central Iceland collapsed from August 2014 to February 2015 during the largest eruption in Europe since 1784. An ice-filled subsidence bowl, 110 square kilometers (km2) in area and up to 65 meters (m) deep developed, while magma drained laterally for 48 km along a subterranean path and erupted as a major lava flow northeast of the volcano. Our data provide unprecedented insight into the workings of a collapsing caldera. RATIONALE Collapses of caldera volcanoes are, fortunately, not very frequent, because they are often associated with very large volcanic eruptions. On the other hand, the rarity of caldera collapses limits insight into this major geological hazard. Since the formation of Katmai caldera in 1912, during the 20th century’s largest eruption, only five caldera collapses are known to have occurred before that at Bárdarbunga. We used aircraft-based altimetry, satellite photogrammetry, radar interferometry, ground-based GPS, evolution of seismicity, radio-echo soundings of ice thickness, ice flow modeling, and geobarometry to describe and analyze the evolving subsidence geometry, its underlying cause, the amount of magma erupted, the geometry of the subsurface caldera ring faults, and the moment tensor solutions of the collapse-related earthquakes. RESULTS After initial lateral withdrawal of magma for some days though a magma-filled fracture propagating through Earth’s upper crust, preexisting ring faults under the volcano were reactivated over the period 20 to 24 August, marking the onset of collapse. On 31 August, the eruption started, and it terminated when the collapse stopped, having produced 1.5 km of basaltic lava. The subsidence of the caldera declined with time in a near-exponential manner, in phase with the lava flow rate. The volume of the subsidence bowl was about 1.8 km3. Using radio-echo soundings, we find that the subglacial bedrock surface after the collapse is down-sagged, with no indications of steep fault escarpments. Using geobarometry, we determined the depth of magma reservoir to be ~12 km, and modeling of geodetic observations gives a similar result. High-precision earthquake locations and moment tensor analysis of the remarkable magnitude M5 earthquake series are consistent with steeply dipping ring faults. Statistical analysis of seismicity reveals communication over tens of kilometers between the caldera and the dike. CONCLUSION We conclude that interaction between the pressure exerted by the subsiding reservoir roof and the physical properties of the subsurface flow path explain the gradual near-exponential decline of both the collapse rate and the intensity of the 180-day-long eruption. By combining our various data sets, we show that the onset of collapse was caused by outflow of magma from underneath the caldera when 12 to 20% of the total magma intruded and erupted had flowed from the magma reservoir. However, the continued subsidence was driven by a feedback between the pressure of the piston-like block overlying the reservoir and the 48-km-long magma outflow path. Our data provide better constraints on caldera mechanisms than previously available, demonstrating what caused the onset and how both the roof overburden and the flow path properties regulate the collapse. The Bárdarbunga caldera and the lateral magma flow path to the Holuhraun eruption site. (A) Aerial view of the ice-filled Bárdarbunga caldera on 24 October 2014, view from the north. (B) The effusive eruption in Holuhraun, about 40 km to the northeast of the caldera
Journal of Geophysical Research | 2015
Michelle Parks; James D P Moore; Xanthos Papanikolaou; Juliet Biggs; Tamsin A. Mather; David M. Pyle; Costas Raptakis; Demitris Paradissis; Andrew Hooper; Barry Parsons; Paraskevi Nomikou
Periods of unrest at caldera-forming volcanic systems characterized by increased rates of seismicity and deformation are well documented. Some can be linked to eventual eruptive activity, while others are followed by a return to quiescence. Here we use a 20 year record of interferometric synthetic aperture radar (InSAR) and GPS measurements from Santorini volcano to further our understanding of geodetic signals at a caldera-forming volcano during the periods of both quiescence and unrest, with measurements spanning a phase of quiescence and slow subsidence (1993–2010), followed by a phase of unrest (January 2011 to April 2012) with caldera-wide inflation and seismicity. Mean InSAR velocity maps from 1993–2010 indicate an average subsidence rate of ~6 mm/yr over the southern half of the intracaldera island Nea Kameni. This subsidence can be accounted for by a combination of thermal contraction of the 1866–1870 lava flows and load-induced relaxation of the substrate. For the period of unrest, we use a joint inversion technique to convert InSAR measurements from three separate satellite tracks and GPS observations from 10 continuous sites into a time series of subsurface volume change. The optimal location of the inflating source is consistent with previous studies, situated north of Nea Kameni at a depth of ~4 km. However, the time series reveals two distinct pressure pulses. The first pulse corresponds to a volume change (ΔV) within the shallow magma chamber of (11.56 ± 0.14) × 106 m3, and the second pulse has a ΔV of (9.73 ± 0.10) × 106 m3. The relationship between the timing of these pulses and microseismicity observations suggests that these pulses may be driven by two separate batches of magma supplied to a shallow reservoir. We find no evidence suggesting a change in source location between the two pulses. The decline in the rates of volume change at the end of both pulses and the observed lag of the deformation signal behind cumulative seismicity, suggest a viscoelastic response. We use a simple model to show that two separate pulses of magma intruding into a shallow magma chamber surrounded by a viscoelastic shell can account for the observed temporal variation in cumulative volume change and seismicity throughout the period of unrest. Given the similarities between the geodetic signals observed here and at other systems, this viscoelastic model has potential use for understanding behavior at other caldera systems.
Nature Communications | 2016
Paraskevi Nomikou; Timothy H. Druitt; Christian Hübscher; Tamsin A. Mather; M. Paulatto; L. M. Kalnins; Karim Kelfoun; Dimitrios Papanikolaou; K. Bejelou; Danai Lampridou; David M. Pyle; Steven Carey; A. B. Watts; B.J. Weiß; Michelle Parks
Caldera-forming eruptions of island volcanoes generate tsunamis by the interaction of different eruptive phenomena with the sea. Such tsunamis are a major hazard, but forward models of their impacts are limited by poor understanding of source mechanisms. The caldera-forming eruption of Santorini in the Late Bronze Age is known to have been tsunamigenic, and caldera collapse has been proposed as a mechanism. Here, we present bathymetric and seismic evidence showing that the caldera was not open to the sea during the main phase of the eruption, but was flooded once the eruption had finished. Inflow of water and associated landsliding cut a deep, 2.0–2.5 km3, submarine channel, thus filling the caldera in less than a couple of days. If, as at most such volcanoes, caldera collapse occurred syn-eruptively, then it cannot have generated tsunamis. Entry of pyroclastic flows into the sea, combined with slumping of submarine pyroclastic accumulations, were the main mechanisms of tsunami production.
Geochemistry Geophysics Geosystems | 2015
A. B. Watts; Paraskevi Nomikou; James D P Moore; Michelle Parks; M. Alexandri
Historical bathymetric charts are a potential resource for better understanding the dynamics of the seafloor and the role of active processes, such as submarine volcanism. The British Admiralty, for example, have been involved in lead line measurements of seafloor depth since the early 1790s. Here, we report on an analysis of historical charts in the region of Santorini volcano, Greece. Repeat lead line surveys in 1848, late 1866, and 1925–1928 as well as multibeam swath bathymetry surveys in 2001 and 2006 have been used to document changes in seafloor depth. These data reveal that the flanks of the Kameni Islands, a dacitic dome complex in the caldera center, have shallowed by up to ∼175 m and deepened by up to ∼80 m since 1848. The largest shallowing occurred between the late 1866 and 1925–1928 surveys and the largest deepening occurred during the 1925–1928 and 2001 and 2006 surveys. The shallowing is attributed to the emplacement of lavas during effusive eruptions in both 1866–1870 and 1925–1928 at rates of up to 0.18 and 0.05 km3 a−1, respectively. The deepening is attributed to a load-induced viscoelastic stress relaxation following the 1866–1870 and 1925–1928 lava eruptions. The elastic thickness and viscosity that best fits the observed deepening are 1.0 km and ∼1016 Pa s, respectively. This parameter pair, which is consistent with the predictions of a shallow magma chamber thermal model, explains both the amplitude and wavelength of the historical bathymetric data and the present day rate of subsidence inferred from InSAR analysis.
Archive | 2018
Freysteinn Sigmundsson; Michelle Parks; Rikke Pedersen; Kristín Jónsdóttir; Benedikt Ofeigsson; Ronni Grapenthin; Stéphanie Dumont; Páll Einarsson; Vincent Drouin; Elías Rafn Heimisson; Magnús Tumi Guðmundsson; Halldor Geirsson; Sigrún Hreinsdóttir; Erik Sturkell; Andrew Hooper; Þórdís Högnadóttir; Kristín S. Vogfjörð; Talfan Barnie; Matthew J. Roberts
Abstract Improving our understanding of volcanic hazards requires better knowledge of the location, volume and properties of magma bodies in the roots of active volcanoes, as well as information on melt supply and magma transfer. This requires a good understanding of both the geometric structure of the volcanic and igneous plumbing system, as well as observations of sub-surface magma movements and their interpretation. Arrival of new magma in volcano roots often causes volcanic unrest expressed by one or more of the following: increased seismicity, ground deformation, volcanic gas release and ground temperature changes. Recent eruptions and magmatic events in Iceland have provided opportunities to apply repeated geodetic observations at volcanoes to measure ground deformation and interpret these measurements together with seismic observations in terms of subsurface magmatic processes.
ieee asia pacific conference on synthetic aperture radar | 2015
Matthew C. Garthwaite; Sarah Lawrie; Steve J. Saunders; Suame Ampana; Michelle Parks
In this contribution we present interferometric time series analysis of ALOS PALSAR images acquired between 2007 and 2011 for the Rabaul Caldera, situated at the north-eastern point of New Britain Island in Papua New Guinea. During this time period, a broad subsidence signal is observed across the caldera, followed by a period of uplift. These signals are thought to originate from deflation and inflation (respectively) from a magma chamber situated at 4.258°S, 152.182°E and a depth of 4.5 km beneath Rabaul Harbor. Using a Mogi point source model, we infer the time series of volume change in this magma chamber and deduce a deflation rate of ~10×10<sup>6</sup> m<sup>3</sup> yr<sup>-1</sup> during 2008 and 2009 and an inflation rate of ~7×10<sup>6</sup> m<sup>3</sup> yr<sup>-1</sup> during 2010 and early 2011.
Nature | 2015
Freysteinn Sigmundsson; Andrew Hooper; Sigrún Hreinsdóttir; Kristin S. Vogfjord; Benedikt Ofeigsson; Elías Rafn Heimisson; Stéphanie Dumont; Michelle Parks; Karsten Spaans; Gunnar B. Gudmundsson; Vincent Drouin; Thóra Árnadóttir; Kristín Jónsdóttir; Magnús T. Gudmundsson; Thórdís Högnadóttir; Hildur María Fridriksdóttir; Martin Hensch; Páll Einarsson; Eyjólfur Magnússon; Sergey V. Samsonov; Bryndís Brandsdóttir; Robert S. White; Thorbjörg Ágústsdóttir; Tim Greenfield; Robert G. Green; Rikke Pedersen; Richard A. Bennett; Halldór Geirsson; Peter La Femina; Helgi Björnsson
Nature Geoscience | 2012
Michelle Parks; Juliet Biggs; Philip England; Tamsin A. Mather; Paraskevi Nomikou; Kirill S. Palamartchouk; Xanthos Papanikolaou; Demitris Paradissis; Barry Parsons; David M. Pyle; Costas Raptakis; Vangelis Zacharis
Earth and Planetary Science Letters | 2013
Michelle Parks; Stefano Caliro; Giovanni Chiodini; David M. Pyle; Tamsin A. Mather; Kim Berlo; Marie Edmonds; Juliet Biggs; Paraskevi Nomikou; Costas Raptakis
Journal of Volcanology and Geothermal Research | 2011
Michelle Parks; Juliet Biggs; Tamsin A. Mather; D.P. Pyle; Falk Amelung; Maribel Monsalve; L. Narvaez Medina