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dc.contributor.authorAsano, Kimiyukien
dc.contributor.authorSekiguchi, Harukoen
dc.contributor.authorIwata, Tomotakaen
dc.contributor.authorYoshimi, Masayukien
dc.contributor.authorHayashida, Takumien
dc.contributor.authorSaomoto, Hidetakaen
dc.contributor.authorHorikawa, Haruoen
dc.contributor.alternative浅野, 公之ja
dc.contributor.alternative関口, 春子ja
dc.contributor.alternative岩田, 知孝ja
dc.contributor.alternative吉見, 雅行ja
dc.contributor.alternative林田, 拓己ja
dc.contributor.alternative竿本, 英貴ja
dc.contributor.alternative堀川, 晴央ja
dc.date.accessioned2017-07-05T00:44:05Z-
dc.date.available2017-07-05T00:44:05Z-
dc.date.issued2016-02-01-
dc.identifier.issn0956-540X-
dc.identifier.urihttp://hdl.handle.net/2433/226323-
dc.description.abstractOn 2013 April 13, an inland earthquake of Mw 5.8 occurred in Awaji Island, which forms the western boundary of the Osaka sedimentary basin in western Japan. The strong ground motion data were collected from more than 100 stations within the basin and it was found that in the Osaka Plain, the pseudo velocity response spectra at a period of around 6.5 s were significantly larger than at other stations of similar epicentral distance outside the basin. The ground motion lasted longer than 3 min in the Osaka Plain where its bedrock depth spatially varies from approximately 1 to 2 km. We modelled long-period (higher than 2 s) ground motions excited by this earthquake, using the finite difference method assuming a point source, to validate the present velocity structure model and to obtain better constraint of the attenuation factor of the sedimentary part of the basin. The effect of attenuation in the simulation was included in the form of Q(f) = Q0(f/f0), where Q0 at a reference frequency f0 was given by a function of the S-wave velocity, Q0 = αVS. We searched for appropriate Q0 values by changing α for a fixed value of f0 = 0.2 Hz. It was found that values of α from 0.2 to 0.5 fitted the observations reasonably well, but that the value of α = 0.3 performed best. Good agreement between the observed and simulated velocity waveforms was obtained for most stations within the Osaka Basin in terms of both amplitude and ground motion duration. However, underestimation of the pseudo velocity response spectra in the period range of 5–7 s was recognized in the central part of the Osaka Plain, which was caused by the inadequate modelling of later phases or wave packets in this period range observed approximately 2 min after the direct S-wave arrival. We analysed this observed later phase and concluded that it was a Love wave originating from the direction of the east coast of Awaji Island.en
dc.format.mimetypeapplication/pdf-
dc.language.isoeng-
dc.publisherOxford University Press (OUP)en
dc.rightsThis article has been accepted for publication in 'Geophysical Journal International' © The Authors 2016. Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved.en
dc.subjectEarthquake ground motionsen
dc.subjectSeismic attenuationen
dc.subjectSite effectsen
dc.subjectComputational seismologyen
dc.subjectWave propagationen
dc.titleModelling of wave propagation and attenuation in the Osaka sedimentary basin, western Japan, during the 2013 Awaji Island earthquakeen
dc.typejournal article-
dc.type.niitypeJournal Article-
dc.identifier.jtitleGeophysical Journal Internationalen
dc.identifier.volume204-
dc.identifier.issue3-
dc.identifier.spage1678-
dc.identifier.epage1694-
dc.relation.doi10.1093/gji/ggv543-
dc.textversionpublisher-
dcterms.accessRightsopen access-
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