scholarly journals Mechanical and topographic factors influencing lava dome growth and collapse

2021 ◽  
Vol 420 ◽  
pp. 107398
Author(s):  
Claire E. Harnett ◽  
Michael J. Heap
1982 ◽  
Vol 14 (3-4) ◽  
pp. 199-222 ◽  
Author(s):  
Herbert E. Huppert ◽  
John B. Shepherd ◽  
R. Haraldur Sigurdsson ◽  
Stephen J. Sparks
Keyword(s):  

Author(s):  
A. J. Hale ◽  
L. Bourgouin ◽  
H. B. Mühlhaus

2013 ◽  
Vol 259 ◽  
pp. 308-316 ◽  
Author(s):  
Angela K. Diefenbach ◽  
Katharine F. Bull ◽  
Rick L. Wessels ◽  
Robert G. McGimsey
Keyword(s):  

2019 ◽  
Vol 7 ◽  
Author(s):  
Edgar U. Zorn ◽  
Nicolas Le Corvec ◽  
Nick R. Varley ◽  
Jacqueline T. Salzer ◽  
Thomas R. Walter ◽  
...  

2021 ◽  
Author(s):  
Martin Mergili ◽  
Shiva P. Pudasaini

<p>An active phase of Soufrière Hills Volcano (Montserrat, Lesser Antilles) has started in 1995 and had its most intense period between 1995 and 2010, when phases of lava dome growth were interrupted by dome collapses triggering ash clouds and different types of pyroclastic flows. These flows were released in various directions, so that two thirds of the island were left in an inhabitable state. The material deposited was later remobilized through lahar flows, burying the centre of the former capital town of Plymouth. In the present work, we attempt to back-calculate the sequences of dome growth – pyroclastic flows, and the subsequent lahar flows, in an integrated way, using the mass flow simulation tool r.avaflow. Thereby, we build on the reconstruction of the pre-event topography as well as on various reference data obtained from the large amount of available literature – mainly, the peak elevation and volumes of the lava domes, the impact areas of the flow processes, and ash fall characteristics. Most observations are successfully reproduced with physically plausible, though calibrated, parameter sets and temporal scaling of lava dome growth. Due to the complexity and multi-stage nature of the volcanic crisis, a number of simplifications had to be introduced, such as considering only the twelve largest sequences of dome growth and pyroclastic flows, and evaluating some of the results on the basis of aggregated impact areas for more than one event. Consequently, the results reflect a strong conceptual component, but can - at least in part - be considered useful for predictive modelling of similar events. Another scope of the simulation results, however, is its educational use. Appropriately presented, they greatly facilitate the generation of a better understanding for complex chains of volcanic processes and their consequences to learners at various levels in different educational contexts, from school and university all the way to targeted awareness-building campaigns.</p>


2007 ◽  
Vol 170 (3) ◽  
pp. 1431-1438 ◽  
Author(s):  
Laurent Bourgouin ◽  
Hans-Bernd Mühlhaus ◽  
Alina Jane Hale ◽  
Antonin Arsac

2021 ◽  
Vol 9 ◽  
Author(s):  
Caroline Martel ◽  
Michel Pichavant ◽  
Hélène Balcone-Boissard ◽  
Georges Boudon

A prerequisite in refining volcanic hazard at explosive volcanoes is a better quantification of the timescales of the syn-eruptive processes, such as magma degassing and crystallization prior to eruption. To this aim, new data on the matrices (microlites, residual glasses, and bubbles) of pumice, scoria, and dense clasts erupted during the AD 1530 andesitic eruption of La Soufrière of Guadeloupe are combined with published data from phase-equilibrium and kinetic experiments, in order to estimate pressures of microlite crystallization and magma ascent rates. From the timescale data, we infer that the AD 1530 eruption started with phreatomagmatic explosions tapping magmas that ascended during about 1 month (decompression rate of ∼50 Pa/s) from the coldest parts of the reservoir (∼825°C and a 74 wt% SiO2 melt). These magmas continuously crystallized microlites (∼25 vol% plagioclase, orthopyroxene, clinopyroxene, magnetite, quartz, and apatite), but did not outgas likely due to sealed conduit margins. The flank collapse (preexisting “cold” edifice) that followed the phreatomagmatic phase triggered a sub-Plinian eruption that progressively tapped the hotter main reservoir (∼875°C and 71 wt% SiO2 interstitial melt), emitting banded and homogeneous pumice. The banded pumice did not significantly outgas and mostly lack decompression-induced microlites, suggesting short ascent durations of the order of 0.5–1 day (decompression rates of 1,400–4,000 Pa/s). The following Strombolian phase emitted dark scoria that did not significantly outgas and only crystallized rare microlites, suggesting ascent duration of the order of 2 days (decompression rates of ∼550 Pa/s). The terminal lava dome growth involved fully outgassed magmas ascended during more than 1 month, giving time for microlite crystallization (∼40 vol% plagioclase, orthopyroxene, clinopyroxene, magnetite, and cristobalite). The detection of any shallow new magmatic intrusion is crucial, since it can trigger a sequence of conduit processes leading to an eruption marked by a succession of different and disastrous eruptive styles, following a scenario similar to the AD 1530 eruption. Overall, we provide a combined approach of petrological, geochemical, and experimental data that may be used to infer ascent conditions and rates at other volcanic systems.


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