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We performed textural (bubble and crystal) and compositional analyses of pyroclasts that were obtained from the Tenjo pyroclastic flow, which resulted on account of the eruption in 838 A.D. on Kozu Island, about 200 km south of Tokyo, Japan. Pyroclasts in one flow unit (300 similar to 2,060 kg/m(3); average density 1330 kg/m(3)) can be classified into three types on the basis of vesicle textures. Type I pyroclasts have small isolated spherical bubbles with higher vesicularities (67-77 vol.%) and number density (10.8-11.7 log m(-3)). Type II pyroclasts have vesicularities similar to type I (61-69 vol.%), but most bubbles exhibit evidences of bubble coalescence, and lower number densities than type I (8.9-9.5 log m(-3)). Type III pyroclasts contain highly deformed bubbles with lower vesicularities (16-34 vol.%) and number densities (8.2-9.0 log m(-3)). The microlite volume fraction (DRE converted) also changes consistently across type I, type II, and type III as 0.06, 0.08, and 0.10-0.15, respectively. However, the number density of the microlites remains nearly invariant in all the pyroclast types. These facts indicate that the variation in the microlite volume fraction is controlled not by the number density (i.e., nucleation process), but by the size (i.e., growth process); the growth history of each type of microlite was different. Water content determinations show that the three types of pumices have similar H2O contents (2.6 +/- 0.2wt%). This fact implies that all three types were quenched at nearly the same depth (35 +/- 5 MPa, assuming that the magma was water-saturated) in the conduit. If the crystal sizes are limited only by growth time, a variation in this parameter can be related to the residence time, which is attributed to the flow heterogeneity in the conduit. By assuming a laminar Poiseuille-type flow, these textural observations can be explained by the difference in ascent velocity and shearing motion across the conduit, which in turn results in the differences in growth times of crystals, degrees of deformation, and bubble coalescence. Consequently, for crystals in the inner part of the conduit, the crystal growth time from nucleation to quenching is shorter than that near the conduit wall. 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  1. 防災科研関係論文

Crystallization of microlites and degassing during magma ascent: Constraints on the fluid mechanical behavior of magma during the Tenjo Eruption on Kozu Island, Japan

https://nied-repo.bosai.go.jp/records/4155
https://nied-repo.bosai.go.jp/records/4155
0e23fa1c-3d8e-441f-bc44-4099a51213d5
Item type researchmap(1)
公開日 2023-03-30
タイトル
言語 en
タイトル Crystallization of microlites and degassing during magma ascent: Constraints on the fluid mechanical behavior of magma during the Tenjo Eruption on Kozu Island, Japan
言語
言語 eng
著者 S Noguchi

× S Noguchi

en S Noguchi

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A Toramaru

× A Toramaru

en A Toramaru

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T Shimano

× T Shimano

en T Shimano

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抄録
内容記述タイプ Other
内容記述 Bubble and crystal textures provide information with regard to the kinetics of the vesiculation and crystallization processes. They also provide insights into the fluid mechanical behavior of magma in a conduit. We performed textural (bubble and crystal) and compositional analyses of pyroclasts that were obtained from the Tenjo pyroclastic flow, which resulted on account of the eruption in 838 A.D. on Kozu Island, about 200 km south of Tokyo, Japan. Pyroclasts in one flow unit (300 similar to 2,060 kg/m(3); average density 1330 kg/m(3)) can be classified into three types on the basis of vesicle textures. Type I pyroclasts have small isolated spherical bubbles with higher vesicularities (67-77 vol.%) and number density (10.8-11.7 log m(-3)). Type II pyroclasts have vesicularities similar to type I (61-69 vol.%), but most bubbles exhibit evidences of bubble coalescence, and lower number densities than type I (8.9-9.5 log m(-3)). Type III pyroclasts contain highly deformed bubbles with lower vesicularities (16-34 vol.%) and number densities (8.2-9.0 log m(-3)). The microlite volume fraction (DRE converted) also changes consistently across type I, type II, and type III as 0.06, 0.08, and 0.10-0.15, respectively. However, the number density of the microlites remains nearly invariant in all the pyroclast types. These facts indicate that the variation in the microlite volume fraction is controlled not by the number density (i.e., nucleation process), but by the size (i.e., growth process); the growth history of each type of microlite was different. Water content determinations show that the three types of pumices have similar H2O contents (2.6 +/- 0.2wt%). This fact implies that all three types were quenched at nearly the same depth (35 +/- 5 MPa, assuming that the magma was water-saturated) in the conduit. If the crystal sizes are limited only by growth time, a variation in this parameter can be related to the residence time, which is attributed to the flow heterogeneity in the conduit. By assuming a laminar Poiseuille-type flow, these textural observations can be explained by the difference in ascent velocity and shearing motion across the conduit, which in turn results in the differences in growth times of crystals, degrees of deformation, and bubble coalescence. Consequently, for crystals in the inner part of the conduit, the crystal growth time from nucleation to quenching is shorter than that near the conduit wall. The vesicle texture variation of bubbles in types I, II, and III results from the difference in the deformation history, implying that the effect of degassing occurred primarily towards the conduit wall.
言語 en
書誌情報 en : BULLETIN OF VOLCANOLOGY

巻 68, 号 5, p. 432-449
出版者
言語 en
出版者 SPRINGER
ISSN
収録物識別子タイプ ISSN
収録物識別子 0258-8900
DOI
関連識別子 10.1007/s00445-005-0019-4
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