Please use this identifier to cite or link to this item: http://hdl.handle.net/2122/3095
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dc.contributor.authorallHarris, A. J. L.; Hawaii Institute of Geophysics and Planetologyen
dc.contributor.authorallBailey, J.; Hawaii Institute of Geophysics and Planetologyen
dc.contributor.authorallCalvari, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Catania, Catania, Italiaen
dc.contributor.authorallDehn, J.; Alaska Volcano Observatory, Geophysical Instituteen
dc.date.accessioned2007-12-12T13:00:48Zen
dc.date.available2007-12-12T13:00:48Zen
dc.date.issued2005en
dc.identifier.urihttp://hdl.handle.net/2122/3095en
dc.description.abstractDuring May 2001 we acquired 2016 thermal images over an ~8-h-long period for a section of active lava channel on Mount Etna (Italy). We used these to extract surface temperature and heat-loss profi les and thereby calculate core cooling rates. Flow surface temperatures declined from ~1070 K at the vent to ~930 K at 70 m. Heat losses were dominated by radiation (5 × 104 W m2) and convection (~104 W/m2). These compare with a heat gain from crystallization of 6 × 103 W/m2. The imbalance between sinks and sources gives core cooling (δT/δx) of ~110 K/km. However, cooling rate per unit distance also depends on fl ow conditions, where we distinguished: (1) unimpeded, high-velocity (~0.2 m/s) fl ow with low δT/δx (0.3 K/m); (2) unimpeded, low-velocity (~0.1 m/s) fl ow with higher δT/δx (0.5 K/m); (3) waning, insulated fl ow at low velocity (~0.1 m/s) with low δT/δx (0.3 K/m); and (4) impeded fl ow at low velocity (<0.1 m/s) with higher δT/δx (0.4 K/m). Our data allow us to defi ne three thermal states of fl ow emplacement: insulated, rapid, and protected. Insulated is promoted by the formation of hanging blockages and coherent roofs. During rapid emplacement, higher velocities suppress cooling rates, and δT/δx can be tied to mean velocity (Vmean) by δT/δx = aVmean –b. In the protected case, deeper, narrow channels present a thermally effi cient channel, where δT/δx can be assessed using the ratio of channel width (w) to depth (d) in w/d = aδT/δx–b.en
dc.language.isoEnglishen
dc.publisher.nameGeological Society of Americaen
dc.relation.ispartofSpecial Paper 396en
dc.subjectlava channelen
dc.subjectEtnaen
dc.subjectheat lossen
dc.subjectcoolingen
dc.subjectviscosityen
dc.subjectvelocityen
dc.subjectFLIRen
dc.titleHeat loss measured at a lava channel and its implications for down-channel cooling and rheologyen
dc.typebook chapteren
dc.description.statusPublisheden
dc.type.QualityControlPeer-revieweden
dc.description.pagenumber125-146en
dc.subject.INGV04. Solid Earth::04.08. Volcanology::04.08.06. Volcano monitoringen
dc.description.obiettivoSpecifico1.5. TTC - Sorveglianza dell'attività eruttiva dei vulcanien
dc.description.fulltextreserveden
dc.contributor.authorHarris, A. J. L.en
dc.contributor.authorBailey, J.en
dc.contributor.authorCalvari, S.en
dc.contributor.authorDehn, J.en
dc.contributor.departmentHawaii Institute of Geophysics and Planetologyen
dc.contributor.departmentHawaii Institute of Geophysics and Planetologyen
dc.contributor.departmentIstituto Nazionale di Geofisica e Vulcanologia (INGV), Sezione OE, Catania, Italiaen
item.openairetypebook chapter-
item.cerifentitytypePublications-
item.languageiso639-1en-
item.grantfulltextrestricted-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.fulltextWith Fulltext-
crisitem.author.deptHawai’i Institute of Geophysics and Planetology, University of Hawai’i at Manoa-
crisitem.author.deptIstituto Nazionale di Geofisica e Vulcanologia (INGV), Sezione OE, Catania, Italia-
crisitem.author.orcid0000-0001-8189-5499-
crisitem.author.parentorgIstituto Nazionale di Geofisica e Vulcanologia-
crisitem.classification.parent04. Solid Earth-
crisitem.department.parentorgIstituto Nazionale di Geofisica e Vulcanologia-
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