2002
DOI: 10.1016/s0377-0273(02)00298-6
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Thermal, seismic and infrasonic evidences of variable degassing rates at Stromboli volcano

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Cited by 171 publications
(129 citation statements)
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“…Two further attributes are of significance with respect to the lava lake level, namely the delay time of the infrasound arrival with respect to the seismic one and the frequency content of the infrasound events (Richardson et al, 2014;Johnson et al, 2018). Unfortunately, the delay time information, which is potentially useful for measuring the level of lava in a conduit (Ripepe et al, 2002;Johnson, 2007) is particularly affected by 6 km of propagation through the atmosphere (see section Identification of Repetitive Long-Period (LP) Seismo-Acoustic Events). Moderate variations of the lava lake depth on the order of 80 m are probably not resolvable with the current seismo-acoustic station.…”
Section: Resultsmentioning
confidence: 99%
“…Two further attributes are of significance with respect to the lava lake level, namely the delay time of the infrasound arrival with respect to the seismic one and the frequency content of the infrasound events (Richardson et al, 2014;Johnson et al, 2018). Unfortunately, the delay time information, which is potentially useful for measuring the level of lava in a conduit (Ripepe et al, 2002;Johnson, 2007) is particularly affected by 6 km of propagation through the atmosphere (see section Identification of Repetitive Long-Period (LP) Seismo-Acoustic Events). Moderate variations of the lava lake depth on the order of 80 m are probably not resolvable with the current seismo-acoustic station.…”
Section: Resultsmentioning
confidence: 99%
“…These bubbles grow via diffusion, decompression-based expansion, or coalesce to form non-spherical bubbles, e.g., of spherical-cap morphology [4][5][6], which can transition into Taylor bubbles (also called gas slugs), which nearly span the conduit width, and are of a length greater than, or equal to, the conduit diameter (see Figure 1 for further details on the morphological characteristics of spherical-cap and Taylor bubbles) [4,7,8]. These distinct bubble morphologies give rise to a variety of potential classes of surface degassing activity, specifically, passive degassing of spherical bubbles [2]; puffing, from bursting of non-spherical bubbles or non-over-pressurized Taylor bubbles [9][10][11]; and explosions from over-pressurized Taylor bubbles [12][13][14]. The latter scenario is associated with strombolian volcanism, as manifested on the eponymous Stromboli volcano, Figure 1.…”
Section: Introductionmentioning
confidence: 99%
“…Solid fragments ejected in each explosion have a mass up to 6,000 kg (Ripepe et al, 2002;. During each explosion, gas emission has been estimated as 6-19 kg/s (Allard et al, 1994).…”
Section: Present-day Activitymentioning
confidence: 99%