Impacts of simulated M9 Cascadia subduction zone motions on idealized systems
Ground motions have been simulated for a magnitude 9 (M9) Cascadia Subduction Zone earthquake, which will affect the Puget Lowland region, including cities underlain by the Seattle, Everett, and Tacoma sedimentary basins. The current national seismic maps do not account for the effects of these basi...
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description | Ground motions have been simulated for a magnitude 9 (M9) Cascadia Subduction Zone earthquake, which will affect the Puget Lowland region, including cities underlain by the Seattle, Everett, and Tacoma sedimentary basins. The current national seismic maps do not account for the effects of these basins on the risk-targeted Maximum Considered Earthquake (MCER). The simulated motions for Seattle had large spectral accelerations (at a period of 2 s, 43% of simulated M9 motions exceeded the MCER), damaging spectral shapes (particularly at periods near 1 s), and long durations (5%-95% significant durations near 110 s). For periods of 1 s or longer, the resulting deformation demands and collapse likelihood for four sets of single-degree-of-freedom systems exceeded the corresponding values for motions consistent with the conditional mean spectra at the MCER intensity (MCER). The regional variation of damage was estimated by combining probabilistic characterizations of the seismic resistance of structures and of the effective spectral acceleration, Sa,eff, which accounts for the effects of spectral acceleration, spectral shape, and ground-motion duration. For high-strength, low-ductility systems located above deep basins (Z2.5> 6 km), the likelihood of collapse during an M9 earthquake averaged 13% and 18% at 1.0 s and 2.0 s periods, respectively. For low-strength, high-ductility systems, the corresponding likelihoods of collapse averaged 18% and 7%. |
doi_str_mv | 10.1193/052418EQS123M |
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The current national seismic maps do not account for the effects of these basins on the risk-targeted Maximum Considered Earthquake (MCER). The simulated motions for Seattle had large spectral accelerations (at a period of 2 s, 43% of simulated M9 motions exceeded the MCER), damaging spectral shapes (particularly at periods near 1 s), and long durations (5%-95% significant durations near 110 s). For periods of 1 s or longer, the resulting deformation demands and collapse likelihood for four sets of single-degree-of-freedom systems exceeded the corresponding values for motions consistent with the conditional mean spectra at the MCER intensity (MCER). The regional variation of damage was estimated by combining probabilistic characterizations of the seismic resistance of structures and of the effective spectral acceleration, Sa,eff, which accounts for the effects of spectral acceleration, spectral shape, and ground-motion duration. For high-strength, low-ductility systems located above deep basins (Z2.5> 6 km), the likelihood of collapse during an M9 earthquake averaged 13% and 18% at 1.0 s and 2.0 s periods, respectively. For low-strength, high-ductility systems, the corresponding likelihoods of collapse averaged 18% and 7%.</description><identifier>ISSN: 8755-2930</identifier><identifier>EISSN: 1944-8201</identifier><identifier>DOI: 10.1193/052418EQS123M</identifier><language>eng</language><publisher>London, England: Earthquake Engineering Research Institute</publisher><subject>Cascadia subduction zone ; earthquakes ; finite difference analysis ; geologic hazards ; great earthquakes ; ground motion ; magnitude ; megathrust earthquakes ; natural hazards ; seismic response ; seismic risk ; Seismology ; simulation ; subduction zones ; United States ; velocity ; Washington</subject><ispartof>Earthquake spectra, 2019-08, Vol.35 (3), p.1261-1287</ispartof><rights>GeoRef, Copyright 2021, American Geosciences Institute. Reference includes data from GeoScienceWorld @Alexandria, VA @USA @United States</rights><rights>2019 Earthquake Engineering Research Institute</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a331t-94f6ed4e1fadfd65f282626a791b4a213b775f2c2dc6d8c9713bbe2e7e527a8c3</citedby><cites>FETCH-LOGICAL-a331t-94f6ed4e1fadfd65f282626a791b4a213b775f2c2dc6d8c9713bbe2e7e527a8c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://journals.sagepub.com/doi/pdf/10.1193/052418EQS123M$$EPDF$$P50$$Gsage$$H</linktopdf><linktohtml>$$Uhttps://journals.sagepub.com/doi/10.1193/052418EQS123M$$EHTML$$P50$$Gsage$$H</linktohtml><link.rule.ids>315,781,785,21824,27929,27930,43626,43627</link.rule.ids></links><search><creatorcontrib>Marafi, Nasser A</creatorcontrib><creatorcontrib>Eberhard, Marc O</creatorcontrib><creatorcontrib>Berman, Jeffrey W</creatorcontrib><creatorcontrib>Wirth, Erin A</creatorcontrib><creatorcontrib>Frankel, Arthur D</creatorcontrib><title>Impacts of simulated M9 Cascadia subduction zone motions on idealized systems</title><title>Earthquake spectra</title><description>Ground motions have been simulated for a magnitude 9 (M9) Cascadia Subduction Zone earthquake, which will affect the Puget Lowland region, including cities underlain by the Seattle, Everett, and Tacoma sedimentary basins. The current national seismic maps do not account for the effects of these basins on the risk-targeted Maximum Considered Earthquake (MCER). The simulated motions for Seattle had large spectral accelerations (at a period of 2 s, 43% of simulated M9 motions exceeded the MCER), damaging spectral shapes (particularly at periods near 1 s), and long durations (5%-95% significant durations near 110 s). For periods of 1 s or longer, the resulting deformation demands and collapse likelihood for four sets of single-degree-of-freedom systems exceeded the corresponding values for motions consistent with the conditional mean spectra at the MCER intensity (MCER). The regional variation of damage was estimated by combining probabilistic characterizations of the seismic resistance of structures and of the effective spectral acceleration, Sa,eff, which accounts for the effects of spectral acceleration, spectral shape, and ground-motion duration. For high-strength, low-ductility systems located above deep basins (Z2.5> 6 km), the likelihood of collapse during an M9 earthquake averaged 13% and 18% at 1.0 s and 2.0 s periods, respectively. For low-strength, high-ductility systems, the corresponding likelihoods of collapse averaged 18% and 7%.</description><subject>Cascadia subduction zone</subject><subject>earthquakes</subject><subject>finite difference analysis</subject><subject>geologic hazards</subject><subject>great earthquakes</subject><subject>ground motion</subject><subject>magnitude</subject><subject>megathrust earthquakes</subject><subject>natural hazards</subject><subject>seismic response</subject><subject>seismic risk</subject><subject>Seismology</subject><subject>simulation</subject><subject>subduction zones</subject><subject>United States</subject><subject>velocity</subject><subject>Washington</subject><issn>8755-2930</issn><issn>1944-8201</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp1kE1Lw0AQhhdRsFaP3vesRPcrH3uUUmuhRUQ9h83ubNmSZEsmQdpfb0oF8eBphpfnGYaXkFvOHjjX8pGlQvFi_vbOhVyfkQnXSiWFYPycTIo8TROhJbskV4hbxnimGJuQ9bLZGdsjjZ5iaIba9ODoWtOZQWtcMBSHyg22D7Glh9gCbeJxH4WWBgemDodRwD320OA1ufCmRrj5mVPy-Tz_mL0kq9fFcva0SoyUvE-08hk4Bdwb512WelGITGQm17xSRnBZ5fkYWuFs5gqr8zGpQEAOqchNYeWUJKe7touIHfhy14XGdPuSs_LYRfmni5G_O_FoNlBu49C143v_wvcneAMRbYDWwlfsavfrCSZ4yZjWqZbfsCZuMQ</recordid><startdate>20190801</startdate><enddate>20190801</enddate><creator>Marafi, Nasser A</creator><creator>Eberhard, Marc O</creator><creator>Berman, Jeffrey W</creator><creator>Wirth, Erin A</creator><creator>Frankel, Arthur D</creator><general>Earthquake Engineering Research Institute</general><general>SAGE Publications</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20190801</creationdate><title>Impacts of simulated M9 Cascadia subduction zone motions on idealized systems</title><author>Marafi, Nasser A ; Eberhard, Marc O ; Berman, Jeffrey W ; Wirth, Erin A ; Frankel, Arthur D</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a331t-94f6ed4e1fadfd65f282626a791b4a213b775f2c2dc6d8c9713bbe2e7e527a8c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Cascadia subduction zone</topic><topic>earthquakes</topic><topic>finite difference analysis</topic><topic>geologic hazards</topic><topic>great earthquakes</topic><topic>ground motion</topic><topic>magnitude</topic><topic>megathrust earthquakes</topic><topic>natural hazards</topic><topic>seismic response</topic><topic>seismic risk</topic><topic>Seismology</topic><topic>simulation</topic><topic>subduction zones</topic><topic>United States</topic><topic>velocity</topic><topic>Washington</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Marafi, Nasser A</creatorcontrib><creatorcontrib>Eberhard, Marc O</creatorcontrib><creatorcontrib>Berman, Jeffrey W</creatorcontrib><creatorcontrib>Wirth, Erin A</creatorcontrib><creatorcontrib>Frankel, Arthur D</creatorcontrib><collection>CrossRef</collection><jtitle>Earthquake spectra</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Marafi, Nasser A</au><au>Eberhard, Marc O</au><au>Berman, Jeffrey W</au><au>Wirth, Erin A</au><au>Frankel, Arthur D</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Impacts of simulated M9 Cascadia subduction zone motions on idealized systems</atitle><jtitle>Earthquake spectra</jtitle><date>2019-08-01</date><risdate>2019</risdate><volume>35</volume><issue>3</issue><spage>1261</spage><epage>1287</epage><pages>1261-1287</pages><issn>8755-2930</issn><eissn>1944-8201</eissn><abstract>Ground motions have been simulated for a magnitude 9 (M9) Cascadia Subduction Zone earthquake, which will affect the Puget Lowland region, including cities underlain by the Seattle, Everett, and Tacoma sedimentary basins. The current national seismic maps do not account for the effects of these basins on the risk-targeted Maximum Considered Earthquake (MCER). The simulated motions for Seattle had large spectral accelerations (at a period of 2 s, 43% of simulated M9 motions exceeded the MCER), damaging spectral shapes (particularly at periods near 1 s), and long durations (5%-95% significant durations near 110 s). For periods of 1 s or longer, the resulting deformation demands and collapse likelihood for four sets of single-degree-of-freedom systems exceeded the corresponding values for motions consistent with the conditional mean spectra at the MCER intensity (MCER). The regional variation of damage was estimated by combining probabilistic characterizations of the seismic resistance of structures and of the effective spectral acceleration, Sa,eff, which accounts for the effects of spectral acceleration, spectral shape, and ground-motion duration. For high-strength, low-ductility systems located above deep basins (Z2.5> 6 km), the likelihood of collapse during an M9 earthquake averaged 13% and 18% at 1.0 s and 2.0 s periods, respectively. For low-strength, high-ductility systems, the corresponding likelihoods of collapse averaged 18% and 7%.</abstract><cop>London, England</cop><pub>Earthquake Engineering Research Institute</pub><doi>10.1193/052418EQS123M</doi><tpages>27</tpages></addata></record> |
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subjects | Cascadia subduction zone earthquakes finite difference analysis geologic hazards great earthquakes ground motion magnitude megathrust earthquakes natural hazards seismic response seismic risk Seismology simulation subduction zones United States velocity Washington |
title | Impacts of simulated M9 Cascadia subduction zone motions on idealized systems |
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