Daniel J. Ponti
United States Geological Survey
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Bulletin of the Seismological Society of America | 2003
David M. Boore; James F. Gibbs; William B. Joyner; John C. Tinsley; Daniel J. Ponti
We have estimated ground motions at the site of a bridge collapse during the 1994 Northridge, California, earthquake. The estimated motions are based on correcting motions recorded during the mainshock 2.3 km from the collapse site for the relative site response of the two sites. Shear-wave slownesses and damping based on analysis of borehole measurements at the two sites were used in the site response analysis. We estimate that the motions at the collapse site were probably larger, by factors ranging from 1.2 to 1.6, than at the site at which the ground motion was recorded, for periods less than about 1 sec.
Journal of Geophysical Research | 1997
Carol S. Prentice; Daniel J. Ponti
The Wrights tunnel is an abandoned railroad tunnel that crosses the San Andreas fault in the southern Santa Cruz Mountains in the vicinity of the 1989 Loma Prieta earthquake. The tunnel was damaged and deformed during the 1906 San Francisco earthquake and a plot showing postearthquake measurements made in the tunnel is given by Lawson [1908]. The amount of offset shown on this plot (1.5 m) has been used in several studies as being representative of the amount of fault offset along this segment of the San Andreas fault in 1906. Our historical research shows that different observers reported different amounts of fault offset in the tunnel and that the 1.5 m given on the plot is not a surveyed measurement. In addition, the plot of the tunnel has been interpreted in several previous studies as evidence of a broad (1.5 km) zone of faulting beneath Summit Ridge. Our analysis shows that this plot need not indicate a broad zone of deformation. Our historical research and modeling of the tunnel measurements indicate that faulting was confined to a zone less than 400 m wide and that 60–85% of the coseismic slip occurred across a single fault plane. There is no evidence for offset across a second shear zone beneath Summit Ridge in 1906. This implies that surface fractures reported on Summit Ridge in 1906 were not associated with significant deformation of the tunnel, implying that they were shallow, surficial features. By analogy, the very similar fractures that occurred on Summit Ridge in 1989 were also probably the result of shallow gravitational, rather than deep-seated tectonic, processes. Our modeling also indicates that total coseismic, near-surface slip across the San Andreas fault zone in the Wrights tunnel in 1906 was at least 1.7–1.8 m.
Earthquake Spectra | 2011
Keith Porter; Lucile M. Jones; Dale Cox; James D. Goltz; Kenneth W. Hudnut; Dennis S. Mileti; Sue A. Perry; Daniel J. Ponti; Michael Reichle; Adam Rose; Charles Scawthorn; Hope A. Seligson; Kimberley I. Shoaf; Jerry Treiman; Anne Wein
In 2008, an earthquake-planning scenario document was released by the U.S. Geological Survey (USGS) and California Geological Survey that hypothesizes the occurrence and effects of a Mw7.8 earthquake on the southern San Andreas Fault. It was created by more than 300 scientists and engineers. Fault offsets reach 13 m and up to 8 m at lifeline crossings. Physics-based modeling was used to generate maps of shaking intensity, with peak ground velocities of 3 m/sec near the fault and exceeding 0.5 m/sec over 10,000 km2. A custom HAZUS®MH analysis and 18 special studies were performed to characterize the effects of the earthquake on the built environment. The scenario posits 1,800 deaths and 53,000 injuries requiring emergency room care. Approximately 1,600 fires are ignited, resulting in the destruction of 200 million square feet of the building stock, the equivalent of 133,000 single-family homes. Fire contributes
Geology | 2017
Kristian J. Bergen; John H. Shaw; Lorraine A. Leon; James F. Dolan; Thomas L. Pratt; Daniel J. Ponti; Eric M. Morrow; Wendy Barrera; Edward J. Rhodes; Madhav K. Murari; Lewis A. Owen
87 billion in property and business interruption loss, out of the total
Earth and Space Science | 2016
Stephen B. DeLong; Andrea Donnellan; Daniel J. Ponti; Ron S. Rubin; James J. Lienkaemper; Carol S. Prentice; Timothy E. Dawson; Gordon G. Seitz; David P. Schwartz; Kenneth W. Hudnut; Carla M. Rosa; Jay Parker
191 billion in economic loss, with most of the rest coming from shake-related building and content damage (
Earthquake Spectra | 2011
Jerome A. Treiman; Daniel J. Ponti
46 billion) and business interruption loss from water outages (
Science | 1994
Lucile M. Jones; Keiiti Aki; David M. Boore; Mehmet Çelebi; Andrea Donnellan; John F. Hall; Ruth A. Harris; Egill Hauksson; Thomas H. Heaton; Susan E. Hough; Kenneth W. Hudnut; K. Hutton; M. J. S. Johnston; W. Joyner; Hiroo Kanamori; G. Marshall; Andrew J. Michael; Jim Mori; M. Murray; Daniel J. Ponti; Paul A. Reasenberg; David P. Schwartz; Leonardo Seeber; A. Shakal; Robert W. Simpson; Hong-Kie Thio; John C. Tinsley; M. Todorovska; Mihailo D. Trifunac; David J. Wald
24 billion). Emergency response activities are depicted in detail, in an innovative grid showing activities versus time, a new format introduced in this study.
Bulletin of the Seismological Society of America | 1989
Robert V. Sharp; Karin E. Budding; John Boatwright; M. J. Ader; Manuel G. Bonilla; Malcolm M. Clark; Thomas E. Fumal; K. K. Harms; James J. Lienkaemper; Douglas M. Morton; B. J. O'Neill; C. L. Ostergren; Daniel J. Ponti; M. J. Rymer; John L. Saxton; John D. Sims
Slip rates represent the average displacement across a fault over time and are essential to estimating earthquake recurrence for probabilistic seismic hazard assessments. We demonstrate that the slip rate on the western segment of the Puente Hills blind thrust fault system, which is beneath downtown Los Angeles, California (USA), has accelerated from ∼0.22 mm/yr in the late Pleistocene to ∼1.33 mm/yr in the Holocene. Our analysis is based on syntectonic strata derived from the Los Angeles River, which has continuously buried a fold scarp above the blind thrust. Slip on the fault beneath our field site began during the late-middle Pleistocene and progressively increased into the Holocene. This increase in rate implies that the magnitudes and/or the frequency of earthquakes on this fault segment have increased over time. This challenges the characteristic earthquake model and presents an evolving and potentially increasing seismic hazard to metropolitan Los Angeles.
Open-File Report | 2008
Lucile M. Jones; Richard L. Bernknopf; Dale Cox; James D. Goltz; Kenneth W. Hudnut; Dennis S. Mileti; Suzanne C. Perry; Daniel J. Ponti; Keith Porter; Michael Reichle; Hope A. Seligson; Kimberley I. Shoaf; Jerry Treiman; Anne Wein
The Mw 6.0 South Napa earthquake of 24 August 2014 caused slip on several active fault strands within the West Napa Fault Zone (WNFZ). Field mapping identified 12.5 km of surface rupture. These field observations, near-field geodesy and space geodesy together provide evidence for more than ~30 km of surface deformation with a relatively complex distribution across a number of subparallel lineaments. Along a ~7 km section north of the epicenter, the surface rupture is confined to a single trace that cuts alluvial deposits, reoccupying a low-slope scarp. The rupture continued northward onto at least four other traces through subparallel ridges and valleys. Postseismic slip exceeded coseismic slip along much of the southern part of the main rupture trace with total slip one year post-event approaching 0.5 meters at locations where only a few centimeters were measured the day of the earthquake. Analysis of airborne interferometric synthetic aperture radar data provides slip distributions along fault traces, indicates connectivity and extent of secondary traces, and confirms that postseismic slip only occurred on the main trace of the fault, perhaps indicating secondary structures ruptured as coseismic triggered slip. Previous mapping identified the WNFZ as a zone of distributed faulting, and this was generally borne out by the complex 2014 rupture pattern. Implications for hazard analysis in similar settings include the need to consider the possibility of complex surface rupture in areas of complex topography, especially where multiple potentially Quaternary-active fault strands can be mapped. This article is protected by copyright. All rights reserved.
Journal of Geotechnical and Geoenvironmental Engineering | 1999
Thomas L. Holzer; Michael J. Bennett; Daniel J. Ponti; John C. Tinsley
An earthquake scenario, based on a kinematic rupture model, has been prepared for a Mw 7.8 earthquake on the southern San Andreas Fault. The rupture distribution, in the context of other historic large earthquakes, is judged reasonable for the purposes of this scenario. This model is used as the basis for generating a surface rupture map and for assessing potential direct impacts on lifelines and other infrastructure. Modeling the surface rupture involves identifying fault traces on which to place the rupture, assigning slip values to the fault traces, and characterizing the specific displacements that would occur to each lifeline impacted by the rupture. Different approaches were required to address variable slip distribution in response to a variety of fault patterns. Our results, involving judgment and experience, represent one plausible outcome and are not predictive because of the variable nature of surface rupture.