{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1361699994591215744.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.5194/se-7-1383-2016"}},{"identifier":{"@type":"URI","@value":"https://se.copernicus.org/articles/7/1383/2016/se-7-1383-2016.pdf"}},{"identifier":{"@type":"DOI","@value":"10.5194/sed-7-3053-2015"}},{"identifier":{"@type":"URI","@value":"https://se.copernicus.org/preprints/7/3053/2015/sed-7-3053-2015.pdf"}},{"identifier":{"@type":"HANDLE","@value":"10261/138287"}},{"identifier":{"@type":"HANDLE","@value":"10092/16489"}}],"resourceType":"preprint","dc:title":[{"@value":"Eruptive shearing of tube pumice: pure and simple"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>Abstract. Understanding the physicochemical conditions extant and mechanisms operative during explosive volcanism is essential for reliable forecasting and mitigation of volcanic events. Rhyolitic pumices reflect highly vesiculated magma whose bubbles can serve as a strain indicator for inferring the state of stress operative immediately prior to eruptive fragmentation. Obtaining the full kinematic picture reflected in bubble population geometry has been extremely difficult, involving dissection of a small number of delicate samples. The advent of reliable high-resolution tomography has changed this situation radically. Here we demonstrate via the use of tomography how a statistically powerful picture of the shapes and connectivity of thousands of individual bubbles within a single sample of tube pumice emerges. The strain record of tube pumice is modelled using empirical models of bubble geometry and liquid rheology, reliant on a constraint of magmatic water concentration. FTIR analysis reveals an imbalance in water speciation, suggesting post-eruption hydration, further supported by hydrogen and oxygen isotope measurements. Our work demonstrates that the strain recorded in the tube pumice dominated by simple shear (not pure shear) in the late deformational history of vesicular magma before eruption. This constraint in turn implies that magma ascent is conditioned by a velocity gradient (across the conduit) at the point of origin of tube pumice. Magma ascent accompanied by simple shear should enhance high eruption rates inferred independently for these highly viscous systems.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381699994591215750","@type":"Researcher","foaf:name":[{"@value":"Donald B. Dingwell"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994591215744","@type":"Researcher","foaf:name":[{"@value":"Yan Lavallée"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994591215745","@type":"Researcher","foaf:name":[{"@value":"Kai-Uwe Hess"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994591215751","@type":"Researcher","foaf:name":[{"@value":"Asher Flaws"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994591215746","@type":"Researcher","foaf:name":[{"@value":"Joan Marti"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994591215748","@type":"Researcher","foaf:name":[{"@value":"Alexander R. L. Nichols"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994591215747","@type":"Researcher","foaf:name":[{"@value":"H. Albert Gilg"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994591215749","@type":"Researcher","foaf:name":[{"@value":"Burkhard Schillinger"}]}],"contributor":[{"@id":"https://cir.nii.ac.jp/crid/1893118016175366912","@type":"Researcher","foaf:name":[{"@value":"Consejo Superior de Investigaciones Científicas [https://ror.org/02gfc7t72]"}]},{"@id":"https://cir.nii.ac.jp/crid/1890583643182498695","@type":"Researcher","foaf:name":[{"@value":"European Research Council"}]},{"@id":"https://cir.nii.ac.jp/crid/1890583643182498692","@type":"Researcher","foaf:name":[{"@value":"German Research Foundation"}]}],"publication":{"publicationIdentifier":[{"@type":"EISSN","@value":"18699529"}],"prism:publicationName":[{"@value":"Solid Earth"}],"dc:publisher":[{"@value":"Copernicus GmbH"}],"prism:publicationDate":"2016-09-27","prism:volume":"7","prism:number":"5","prism:startingPage":"1383","prism:endingPage":"1393"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["https://creativecommons.org/licenses/by/3.0/"],"url":[{"@id":"https://se.copernicus.org/articles/7/1383/2016/se-7-1383-2016.pdf"},{"@id":"https://se.copernicus.org/preprints/7/3053/2015/sed-7-3053-2015.pdf"}],"createdAt":"2016-09-27","modifiedAt":"2025-02-08","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Fields%20of%20Research::37%20-%20Earth%20sciences::3705%20-%20Geology::370512%20-%20Volcanology","dc:title":"Fields of Research::37 - Earth sciences::3705 - Geology::370512 - Volcanology"},{"@id":"https://cir.nii.ac.jp/all?q=QE1-996.5","dc:title":"QE1-996.5"},{"@id":"https://cir.nii.ac.jp/all?q=Stratigraphy","dc:title":"Stratigraphy"},{"@id":"https://cir.nii.ac.jp/all?q=Tubes%20(components)","dc:title":"Tubes (components)"},{"@id":"https://cir.nii.ac.jp/all?q=Geology","dc:title":"Geology"},{"@id":"https://cir.nii.ac.jp/all?q=Strain%20indicators","dc:title":"Strain indicators"},{"@id":"https://cir.nii.ac.jp/all?q=QE640-699","dc:title":"QE640-699"},{"@id":"https://cir.nii.ac.jp/all?q=Bubble%20Geometry","dc:title":"Bubble Geometry"},{"@id":"https://cir.nii.ac.jp/all?q=Empirical%20model","dc:title":"Empirical model"},{"@id":"https://cir.nii.ac.jp/all?q=High-resolution%20tomography","dc:title":"High-resolution tomography"},{"@id":"https://cir.nii.ac.jp/all?q=Velocity%20gradients","dc:title":"Velocity gradients"},{"@id":"https://cir.nii.ac.jp/all?q=Physicochemical%20conditions","dc:title":"Physicochemical conditions"},{"@id":"https://cir.nii.ac.jp/all?q=Tomography","dc:title":"Tomography"},{"@id":"https://cir.nii.ac.jp/all?q=Explosive%20volcanism","dc:title":"Explosive volcanism"},{"@id":"https://cir.nii.ac.jp/all?q=Viscous%20systems","dc:title":"Viscous systems"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360294643752230144","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Comparison of Bubble Shape Model Results With Textural Analysis: Implications for the Velocity Profile Across a Volcanic Conduit"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298757438782592","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Reconstruction of submarine eruption processes from FTIR volatile analysis of marine tephra: Example of Oomurodashi volcano, Japan"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567182296115456","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Bubble deformation in magma under transient flow conditions"}]},{"@id":"https://cir.nii.ac.jp/crid/1361131417000563200","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Formation of tube-pumice structure under pure shear: Insights from extension tests of solidifying foam"}]},{"@id":"https://cir.nii.ac.jp/crid/1880865118276286208","@type":"Dataset","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The hydration and alteration of perlite and rhyolite"}]},{"@id":"https://cir.nii.ac.jp/crid/2050870367075052800","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Quantitative measurement of bubble textures in pumice clasts using a digital stereo microscope with low-angled ring illumination"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.5194/se-7-1383-2016"},{"@type":"CROSSREF","@value":"10.5194/sed-7-3053-2015"},{"@type":"OPENAIRE","@value":"doi_dedup___::ed6ac81073058b6fff25723c4f117f8b"},{"@type":"CROSSREF","@value":"10.1186/s40623-020-01320-0_references_DOI_GoqMFVUEeNiuSKAkekSg94zspFf"},{"@type":"CROSSREF","@value":"10.1029/2021jb021841_references_DOI_AubO1jtLqh6LrNWTocf775G162S"},{"@type":"CROSSREF","@value":"10.3389/feart.2022.963392_references_DOI_AubO1jtLqh6LrNWTocf775G162S"},{"@type":"CROSSREF","@value":"10.1016/j.jvolgeores.2020.106772_references_DOI_AubO1jtLqh6LrNWTocf775G162S"},{"@type":"CROSSREF","@value":"10.1016/j.jvolgeores.2018.09.005_references_DOI_GoqMFVUEeNiuSKAkekSg94zspFf"}]}