V008-0014
Characterization of source unsteadiness and entrainment into explosive eruptions using laboratory- and field-based methods

Tuesday, 8 December 2020
Poster
Johanand Gilchrist, University of British Columbia, Earth, Ocean and Atmospheric Sciences, Vancouver, BC, Canada, Cyril Mergny, ENS Lyon, Lyon, France, Colin R R Rowell, University of British Columbia, Earth, Ocean, and Atmospheric Sciences, Vancouver, BC, Canada, Franck Donnadieu, Université Clermont-Auvergne, Clermont, France, Mark Jellinek, Univ British Columbia, Vancouver, BC, Canada, Frédéric Peyrin, Observatoire de Physique du Globe de Clermont-Ferrand, Clermont, France, Thierry Latchimy, Observatoire de Physique du Globe de Clermont-Ferrand, Aubière, France and Julien Delanoë, LATMOS, UVSQ, IPSL, CNRS, Guyancourt, France
Abstract:
Unsteady explosive eruptions are defined by changes in (source conditions) mass flux at the vent occurring on time scales shorter than the rise time of the ash plume. Unsteady eruptions pose daily risks for air traffic and local communities, however, their plume dynamics and spreading heights are poorly understood and represent a critical knowledge gap in volcanology. Development of a classification scheme for the full range of unsteady eruption behavior requires quantification of source unsteadiness and subsequent effects on the entrainment rate, αe, of ambient atmosphere into unsteady ash plumes. Accordingly, we introduce the source Pulsation number (Pu0 = τpe) where τp is the period between pulses of eruption source mass flux and τe the eddy overturn time of the mixture at the source. We expect the full range of explosive eruption plume behavior to occur between endmember “buoyant plumes”, with Pu0 << 1, and “buoyant thermals”, with Pu0 > 1; these regimes are separated by a transitional “connected thermals” regime, with Pu0 1. To test our hypotheses, we deployed a novel portable ground-based L band (3.2 mm wavelength) Doppler radar instrument at Sabancaya Volcano, Peru in 2018 to monitor Vulcanian eruptions over two weeks with unprecedented spatial (12.5 m) and temporal (0.5 s) resolution. We also conduct experiments injecting unsteady fresh water plumes into a density stratified saltwater layer by varying 0 < Pu0 < 1.6 among experiments and estimating αe. Our experimental results confirm that endmember buoyant plume and thermal Pu0 regimes have αe values approaching those found in previous studies for buoyant plumes and thermals, respectively (Figure 1). The transitional “connected thermal” regime occurs where Pu0 ≈ 0.5 and has an αe value between the values of the endmember regimes. Radar data from Sabancaya’s Vulcanian eruptions reveal Pu0 0.8 for eruption pulses detected during semi-continuous eruptive periods. Ongoing work aims to estimate the full range of Pu0 and αe for all eruptions in the radar dataset for comparison with our analog experiment dataset. These results suggest that Pu0 can be used to classify all explosive eruptions, with steady and unsteady source conditions, on one regime diagram.