Development of magnitude-bound relations for paleoliquefaction analyses: New Zealand case study
Introduction
In regions experiencing infrequent moderate-to-large earthquakes, the historic record may be insufficient to provide accurate inputs for seismic hazard analyses because (1) some active faults may be historically seismically quiescent and not easily identifiable from surface evidence, thereby posing an unspecified potential earthquake source, and (2) seismic phenomena such as liquefaction and rockfall may pose a potential hazard but may not have occurred historically. The 2010–2011 Canterbury earthquake sequence (CES) in New Zealand provided a powerful demonstration of these limitations. The CES involved at least 7 damaging earthquakes sourced from at least 12 faults (Beavan et al., 2012) that were previously unidentified and historically seismically quiescent. As many as ten distinct episodes of liquefaction (Quigley et al., 2013) and five distinct episodes of rockfall (Mackey and Quigley, 2014) occurred at some sites in the mainshock (Mw 7.1 Darfield earthquake) and largest aftershocks (e.g., 2011 Mw 6.2 Christchurch earthquake, 185 fatalities). Approximately 75% of buildings within the central business district (CBD) of Christchurch required demolition or extensive repair (Kam et al., 2011). Due to extensive liquefaction-induced land and infrastructure damage, more than 6000 residential properties in eastern Christchurch were purchased by the central government (http://cera.govt.nz/residential-red-zone) at a post-insurance pay out loss exceeding $NZ 1 b ($US 800 m) (Parker and Steenkamp, 2012).
Pre-CES seismic hazard models for the region (e.g., Stirling et al., 2007) that combined regional active faults (source models) with ‘floating’ unidentified sources (distributed seismicity) indicated that (a) proximal, moderate Mw earthquakes from unidentified distributed sources (including blind faults) contributed the largest seismic shaking hazard to Christchurch, (b) earthquakes up to Mw 7.2 on unidentified sources beneath the Canterbury Plains west of Christchurch were possible, and (c) expected return times of potentially liquefaction-inducing peak ground accelerations (PGA ~ 0.1 to 0.2 g) for class C (shallow soil) site conditions ranged from ca. 50 to 200 yr. However, prior to the CES, none of this data had been seriously validated with rigorous paleoseismic investigations in Christchurch. The occurrence of a highly damaging series of earthquakes sourced from previously unknown and primarily blind faults highlighted the inherent incompleteness of source-based seismic hazard catalogs, demonstrating the necessity for geologic studies of prehistoric phenomena such as rockfalls (Mackey and Quigley, 2014) and liquefaction features (Bastin et al., 2015) to supplement seismic hazard models and predict the impacts of future earthquakes. Despite a wealth of recent paleoliquefaction studies in Christchurch (e.g., Almond et al., 2012, Quigley et al., 2013, Bastin et al., 2015, Bastin et al., 2015, Maurer et al., 2014, Villamor et al., 2014), a significant challenge remains in understanding the spatial distribution of earthquake sources and shaking intensities that induced paleo-liquefaction, and are thus capable of inducing future liquefaction, in this region.
Paleoliquefaction studies have two phases. The first phase entails the performance of field investigations, wherein paleoliquefaction features are located, mapped, and dated. The reader is referred to Obermeier et al., 2001, Obermeier et al., 2005 for broad overviews of paleoliquefaction field investigation, and to the intensive investigations by Obermeier and Dickenson (2000), Tuttle (2001), Talwani and Schaeffer (2001), Cox et al. (2004), and Tuttle et al., 2002a, Tuttle et al., 2002b, Tuttle et al., 2005 for specific case studies. The second phase, and the focus of this study, is back-analysis, wherein quantitative techniques are used to determine the magnitude of the causative paleoearthquake and better constrain its source location. Specifically, this study aims to advance the state of the art in back-analysis techniques so that the results of field investigation can be used to accurately assess the paleoseismic history of a region to the extent possible.
Back-analysis techniques have been increasingly applied in paleoliquefaction studies in many seismically active regions (e.g., Obermeier, 1998, Tuttle, 2001, Talwani and Schaeffer, 2001, Cox, 2004, Green et al., 2005, Bastin et al., 2015). While several techniques have been proposed for estimating earthquake magnitudes from paleoliquefaction data, one of the more credible and widely-used is the “magnitude-bound” procedure (e.g., Obermeier, 1998, Olson et al., 2005a, Olson et al., 2005b, Papathanassiou et al., 2005, Pirrotta et al., 2007, Tuttle and Hartleb, 2012). This approach uses correlations relating earthquake magnitude to the site-to-source distance of the most distal observation of liquefaction. Developed from observations in modern earthquakes, these correlations are commonly referred to as magnitude-bound curves. Fig. 1 presents several such correlations for a variety of geographic and tectonic settings (Kuribayahsi and Tatsuoka, 1975, Ambraseys, 1988, Papadopoulos and Lefkopoulos, 1993, Wakamatsu, 1993, Galli, 2000, Aydan et al., 2000, Papathanassiou et al., 2005, Pirrotta et al., 2007, Castilla and Audemard, 2007), where site-to-source distance is quantified in terms of epicentral distance (Fig. 1a) and the distance to most proximal fault rupture (Fig. 1b). The position of these curves, which bound the most distal liquefaction features, is inherently a function of earthquake source characteristics (e.g., rupture mechanism), transmission characteristics (e.g., ground motion attenuation and site effects), and liquefaction susceptibility (e.g., soil state and gradation, and ground water depth). Because these factors vary regionally, region-specific correlations provide more accurate estimates than those developed from global data (Obermeier et al., 2001, Olson et al., 2005a, Olson et al., 2005b).
In addition, inherent to these curves are differing criteria for data inclusion, including the quality and extent of field study, the certainty of earthquake source location and magnitude (e.g., instrumental vs. macroseismic), the style of faulting and focal depth, and the overall anomalousness of data. For example, in developing his curves, Ambraseys (1988) did not consider (1) deep-focus earthquakes, which produce more distal liquefaction than shallow crustal earthquakes; or (2) anomalous cases that would bias the maximum site-to-source distance of liquefaction, including those where conditions greatly enhanced liquefaction susceptibility, such as irrigated fields or sloping ground. Conversely, Castilla and Audemard (2007) included both deep-focus earthquakes and anomalous cases in developing their correlation from global data. For example, Castilla and Audemard (2007) include data from the 1977 Mw7.5 Bucharest, Romania earthquake, having a focal depth of 91–110 km (Ambraseys, 1988, Berg et al., 1980), as well as data from aftershocks following the 1989 Mw5.9 Bova del Tocuyo, Venezuela and Mw6.9 Loma Prieta, USA earthquakes. While further research is needed, it has been shown that surface manifestations of liquefaction may be observed at greater site-to-source distances during aftershocks than in equivalent-magnitude mainshocks, possibly due to increased liquefaction susceptibility from reduced aging-effects, or to the presence of existing liquefaction dikes, which act as conduits between liquefied strata and the ground surface (Green et al., 2013, Maurer et al., 2014). Due to the inclusion of this data, and as shown in Fig. 1a, the Castilla and Audemard (2007) correlation estimates a significantly lower magnitude at shorter site-to-source distances, as compared to using correlations proposed by other authors. Importantly, differing criteria for data selection can result in significant differences to magnitude-bound curves. Therefore, in addition to using regionally-appropriate correlations, familiarity with the provenance of a magnitude-bound curve is critical; to place derivative results in proper context, a user must be aware of a correlation's source data, development, and caveats for use.
While magnitude-bound curves specific to New Zealand have not yet been proposed, there is a clear and present need. In light of the prior inconspicuousness of local faults and the exceedance of design ground-motions during the CES, there is a need to reassess the magnitude-recurrence rates of earthquakes local to Christchurch. Preliminary evidence suggests liquefaction-inducing earthquakes occurred between A.D. 1000 and A.D. 1400 (Villamor et al., 2014) and between AD 1660 – 1803 and ca. 1905 (Bastin et al., 2015) in distinct parts of Christchurch, however the origins of these earthquakes are unknown. The penultimate earthquake on the source of the Darfield earthquake (Greendale Fault) occurred ca. 20–30 kyr ago (Hornblow et al., 2014) and rock fall evidence suggests that no large earthquakes have occurred on the local faults responsible for the 2011 February Mw6.2 and June Mw6.0 Christchurch earthquakes within the last 6000 to 8000 years (Mackey and Quigley, 2014), indicating that the CES sources were not responsible for the paleoliquefaction. Region-specific magnitude-bound curves could thus assist in the interpretation of such evidence and help to elucidate the region's paleoseismic history. As such, the objectives of this study are to: (1) develop a NZ-based magnitude-bound curve using the traditional approach of using modern liquefaction field observations; (2) develop NZ-based magnitude-bound curves using a newly proposed back-calculation approach using the simplified liquefaction evaluation procedure in conjunction with a regionally appropriate ground motion prediction equation (GMPE); and (3) demonstrate the use of these curves by analyzing paleoliquefaction features recently discovered in Christchurch. It is hoped that these correlations ultimately aid in more accurately assessing the regional seismic hazard.
Section snippets
Development of NZ-based magnitude-bound curves
Two approaches are used to develop NZ-based magnitude-bound curves for shallow crustal earthquakes. The first is the traditional approach using modern liquefaction field observations (e.g., Ambraseys, 1988), but based on data from earthquakes in New Zealand only. The second is a newly proposed back-calculation approach using the simplified liquefaction evaluation procedure in conjunction with a regionally appropriate GMPE. In this latter approach both deterministic and probabilistic frameworks
Demonstration of NZ-based magnitude-bound curves
Following the CES, a series of trenches were dug to investigate the structure and stratigraphy of modern, undisturbed liquefaction features (e.g., Green et al., 2012, Quigley et al., 2013). In some cases, trenching also uncovered evidence of paleoliquefaction within the subsurface. One such case is that of Sullivan Park in eastern Christchurch, a site of intensive investigations by Bastin et al., 2013, Bastin et al., 2015. Here, oxidized, pre-CES liquefaction dikes were found to be cross-cut by
Conclusions
To assist in the interpretation of paleoseismic histories, magnitude-bound curves are commonly used to estimate earthquake magnitudes from paleoliquefaction evidence. This study used two independent approaches to develop New Zealand based magnitude-bound curves: (1) using field observational data; and (2) using a back-calculation framework with the simplified liquefaction evaluation procedure and a regionally applicable GMPE, wherein both deterministic and probabilistic frameworks were used.
Acknowledgments
This study is based on work supported by the U.S. National Science Foundation (NSF) grants CMMI-0962952, CMMI-1407428 and CMMI-1435494, and US Geological Survey (USGS) grants G12AP20002 and G14AP00046. However, any opinions, findings, and conclusions or recommendations expressed in this paper are those of the authors and do not necessarily reflect the views of NSF or USGS. The authors also gratefully acknowledge the input from Professor Adrian Rodriguez-Marek at Virginia Tech on computing
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