Please use this identifier to cite or link to this item: http://hdl.handle.net/2122/1944
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dc.contributor.authorallGallovic, F.; Department of Geophysics, Faculty of Mathematics and Physics, Charles University, Prague, V Holesovickach 2, Prague 8, 180 00, Czech Republicen
dc.contributor.authorallBurjanek, J.; Department of Geophysics, Faculty of Mathematics and Physics, Charles University, Prague, V Holesovickach 2, Prague 8, 180 00, Czech Republicen
dc.date.accessioned2006-12-06T16:09:55Zen
dc.date.available2006-12-06T16:09:55Zen
dc.date.issued2006-12-06T16:09:55Zen
dc.identifier.urihttp://hdl.handle.net/2122/1944en
dc.description.abstractWe are investigating two distinct strong ground motion simulation techniques as regards their high-frequency directivity: i) the composite model with a fractal subevent size dis- tribution, based on the method of summation of empirical Green’s functions, and ii) the integral model with the k-squared slip model with k-dependent rise time, based on the representation theorem. We test the simulations in a 1D layered crustal model against em- pirical PGA attenuation relations, particularly with regard to their uncertainty, described by the standard deviation ( ). We assume that any synthetic model for a particular earth- quake should not provide a PGA scatter larger than the observed scatter for a large set of earthquakes. The 1999 Athens earthquake (Mw=5.9) is studied as a test example. In the composite method, the synthetic data display a scatter of less than ±2 around the empirical mean. The k-squared method displays a larger scatter, demonstrating strong high-frequency directivity. It is shown that the latter can be reduced by introducing a formal spectral modification. 1 Introduction Low-frequency directivity effects are well known. For example, there is a number of seismic recordings of recent earthquakes (e.g., 1992 Landers, 1994 Northridge, 1995 Kobe, 1999 Chi-Chi), which show long-period velocity pulses caused by rupture propagation towards a station. This effect can be successfully explained by the apparent source time function varying with azimuth (Haskell, 1964). 2en
dc.format.extent8493508 bytesen
dc.format.mimetypenullen
dc.language.isoEnglishen
dc.subjectdirectivy, strong ground motionsen
dc.titleHigh-Frequency Directivity in Strong Ground Motion Modeling Methodsen
dc.typemanuscripten
dc.description.statusUnpublisheden
dc.subject.INGV04. Solid Earth::04.06. Seismology::04.06.03. Earthquake source and dynamicsen
dc.subject.INGV04. Solid Earth::04.06. Seismology::04.06.04. Ground motionen
dc.description.fulltextopenen
dc.contributor.authorGallovic, F.en
dc.contributor.authorBurjanek, J.en
dc.contributor.departmentDepartment of Geophysics, Faculty of Mathematics and Physics, Charles University, Prague, V Holesovickach 2, Prague 8, 180 00, Czech Republicen
dc.contributor.departmentDepartment of Geophysics, Faculty of Mathematics and Physics, Charles University, Prague, V Holesovickach 2, Prague 8, 180 00, Czech Republicen
item.openairetypemanuscript-
item.cerifentitytypePublications-
item.languageiso639-1en-
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item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
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crisitem.classification.parent04. Solid Earth-
crisitem.classification.parent04. Solid Earth-
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