(1996) formulation is based on just the fundamental frequencypeak, while HVSR in Christchurch often returns two peakscorresponding to resonant strata at different depths; and (2)the K g parameter is dependent on the square of HVSR amplitude,which is quite unstable as discussed before.Finally, the same technique based on S-transform, whichafter the L’Aquila 2009 earthquake did not point out significantevidence of nonlinearity, here shows clear signs of energyat frequencies lower than the fundamental one in the elasticdomain (softening nonlinearity) in the coda of accelerogramsfrom CBGS; at the same time it is possible to recognize hintsof hardening nonlinearity due to hysteretic dilatant behaviorof soils.Future research will include a second, more detailed mappingof soil frequency using HVSR and comparison betweenelastic and nonlinear behavior at all the accelerometric stations,including the recordings of the September 2010 Darfieldearthquake and the June 2011 Christchurch earthquake.ACKNOWLEDGMENTSMany thanks are due to the staff of Canterbury University(Christchurch) who helped with logistical assistance, insightfulfield trips, and stimulating discussions, and in particular toStefano Pampanin, Misko Cubrinovski, Tobias Smith, WengKam, and Umut Akguzel. Thanks to Rocco Ditommaso forthe S-transform calculations. The paper was prepared duringa stay at GFZ–Helmholtz Zentrum, Potsdam, and benefitedfrom comments from colleagues after a seminar presentation.REFERENCESBeroya, M. A. A., A. Aydin, R. Tiglao, and M. Lasala (2009). Use ofmicrotremor in liquefaction hazard mapping. Engineering Geology107, 140–153.Bonilla, L. F., R. J. Archuleta, and D. Lavallée (2005). Histeretic anddilatant behavior of cohesionless soils and their effects on nonlinearsite response: Field data observation and modeling. Bulletin of theSeismological Society of America 95, 2,373– 2,395.Bradley, B. A., and M. Cubrinovski (2011). Near-source strong groundmotions observed in the 22 February 2011 Christchurch earthquake.Seismological Research Letters 82, 853–865.Brown, L. J., and J. H. Weeber (1992). Geology of the Christchurch UrbanArea. Institute of Geological and Nuclear Sciences, Map 1, 1 sheet+ 104 pp. Lower Hutt, New Zealand: GNS Science.Chatelain, J.-L., B. Guillier, F. Cara, A.-M. Duval, K. Atakan, and theSESAME Working Group (2008). Evaluation of the influenceof experimental conditions on H/V results from ambient noiserecordings. Bulletin of Earthquake Engineering 6 (1), 33–74.Cubrinovski, M., and M. Taylor (2011). Liquefaction Map V.1.0 22Feb. 2001 earthquake, http://db.nzsee.org.nz:8080/en/web/chch_2011/geotechnical/-/blogs/liquefaction-map-drive-throughreconnaissance.Last accessed 19 September 2011.Di Giacomo, D., M. R. Gallipoli, M. Mucciarelli, S. Parolai, and S. M.Richwalski (2005). Analysis and modeling of HVSR in the presenceof a velocity inversion: The case of Venosa, Italy. Bulletin of theSeismological Society of America 95, 2,364–2,372.Nakamura, Y. (1996). Real-time information systems for hazard mitigation.In Proceedings of the 10th World Conference in EarthquakeEngineering, paper # 2134.Parolai, S., and S. M. Richwalski (2004). The importance of convertedwaves in comparing H/V and RSM site response estimates. Bulletinof the Seismological Society of America 94 (1), 304–313.Puglia, R., R. Ditommaso, F. Pacor, M. Mucciarelli, L. Luzi, and M.Bianca (2011). Frequency variation in site response as observedfrom strong motion data of the L’Aquila, 2009 seismic sequence.Bulletin of Earthquake Engineering 9 (3), 869–892; doi:10.1007/s10518-011-9266-2.Smyrou, E., P. Tasiopoulou, İ. E. Bal, and G. Gazetas (2011). Groundmotions versus geotechnical and structural damage in the February2011 Christchurch earthquake. Seismological Research Letters 82,882–892.Stockwell, R. G., L. Mansinha, and R. P. Lowe (1996). Localization ofthe complex spectrum: The S transform. IEEE Transactions onSignal Processing 44, 998–1,001.Toshinawa, T., J. J. Taber, and J. B. Berrill (1997). Distribution ofground-motion intensity inferred from questionnaire survey, earthquakerecordings, and microtremor measurements—A case studyin Christchurch, New Zealand, during the 1994 Arthurs Passearthquake, Bulletin of the Seismological Society of America 87 (2),356–369.Department of Structural Engineering, GeotechnicalEngineering, Engineering GeologyBasilicata UniversityViale dell’Ateneo Lucano, 1085100 Potenza Italymarco.mucciarelli@unibas.it926 Seismological Research Letters Volume 82, Number 6 November/December 2011
Use of DCP and SASW Tests to EvaluateLiquefaction Potential: Predictions vs.Observations during the Recent New ZealandEarthquakesRussell A. Green, Clint Wood, Brady Cox, Misko Cubrinovski, Liam Wotherspoon, Brendon Bradley, Thomas Algie, John Allen, Aaron Bradshaw, and Glenn RixRussell A. Green, 1 Clint Wood, 2 Brady Cox, 2 Misko Cubrinovski, 3Liam Wotherspoon, 4 Brendon Bradley, 3 Thomas Algie, 5 John Allen, 6Aaron Bradshaw, 7 and Glenn Rix 8INTRODUCTIONFollowing both the 4 September 2010 M w 7.1 Darfield and22 February 2011 M w 6.2 Christchurch, New Zealand, earthquakes,Geotechnical Extreme Events Reconnaissance (GEER)team members from the United States and New Zealand visitedthe affected areas to assess geotechnical related damage(e.g., Allen et al. 2010a, b). As shown in Figure 1, liquefactionwas pervasive in large portions of the region after both earthquakes.The widespread liquefaction caused extensive damageto residential properties, water and wastewater networks,high-rise buildings, and bridges. For example, nearly 15,000residential houses and properties were severely damaged fromliquefaction and lateral spreading. More than 50% of thesehouses were damaged beyond economic repair. Also, portionsof the central business district (CBD) were severely damagedby liquefaction during the Christchurch earthquake. It is estimatedthat approximately 30% of the buildings in the CBDwere damaged beyond repair, although not all of the damageresulted from liquefaction.Among the field tests performed by the GEER teamwere the dynamic cone penetrometer (DCP) test (Sowers andHedges 1966) and spectral analysis of surface waves (SASW)test (Stokoe et al. 1994). Both of these tests can provide informationabout the liquefaction susceptibility of soil and are relativelyportable, making them suitable for rapid post-earthquakereconnaissance field studies. The objective of this paper is to1. Department of Civil and Environmental Engineering, VirginiaTech, Blacksburg, Virginia U.S.A.2. University of Arkansas, Fayetteville, Arkansas U.S.A.3. University of Canterbury, Christchurch, New Zealand4. University of Auckland, Auckland, New Zealand5. Partners in Performance, Sydney, Australia6. TRI Environmental, Inc., Duluth Minnesota, U.S.A.7. University of Rhode Island, Kingston, Rhode Island, U.S.A.8. Georgia Tech, Atlanta, Georgia, U.S.A.provide an overview of DCP and SASW tests performed acrossthe Christchurch region and to summarize the comparison ofthe observed versus predicted liquefaction occurrence duringboth the Darfield and Christchurch earthquakes.BACKGROUNDAt 4:35 a.m. on 4 September 2010 NZ Standard Time, thepreviously unmapped Greendale fault ruptured, producing theM w 7.1 Darfield earthquake. The epicenter for this event wasapproximately 40 km west of the center of Christchurch, butthe closest distance from the fault rupture to the western suburbsof Christchurch (e.g., Hornby) was only about 10 km (e.g.,Allen et al. 2010a). As shown in Figure 2, representative geometricmeans of the recorded horizontal peak ground accelerations(PGAs) were 0.71 g in the epicentral region, 0.20 g in theCBD, 0.32 g in Kaiapoi (north of Christchurch), and 0.27 gin Lyttelton (south of Christchurch) (e.g., Allen et al. 2010b).The M w 6.2 Christchurch earthquake occurred at 12:51p.m. on 22 February 2011 NZ Standard Time. As with theDarfield earthquake, the Christchurch earthquake occurred ona previously unmapped fault, the Port Hills fault, located in thePort Hills south of Christchurch. The distance from the epicenterto the center of Christchurch was about 8 km, but the ruptureplane was directly beneath some of the southern neighborhoodsof Christchurch (e.g., Heathcote Valley) and Lyttelton.As shown in Figure 2, representative geometric means of therecorded PGAs were 1.31 g in the epicentral region, 0.42 g inthe CBD, 0.20 in Kaiapoi (north of Christchurch), and 0.11 gin Templeton (west of Christchurch).Much of Christchurch and its environs were originallyswampland, beach dune sand, estuaries, and lagoons that weredrained as part of European settlement (Brown et al. 1995).Consequently, in large areas the near-surface soil stratigraphyis characterized by inter-bedded, loose Holocene aged silt,sand, and gravel that are highly susceptible to liquefactiondoi: 10.1785/gssrl.82.6.927Seismological Research Letters Volume 82, Number 6 November/December 2011 927
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News and Notes (continued)Nominatio
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TABLE 1Peak ground acceleration (PG
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Quigley, M., R. Van Dissen, P. Vill
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slip on a 59-degree striking fault
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observations and other source studi
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TABLE 2Solutions for fault location
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-43.45(A)degrees N-43.50-43.552.52.
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is still a good fit to the horizont
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Coulomb Stress Change Sensitivity d
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mation takes on a larger strike-sli
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P 9.4267BLDU45P 20.1213CASY39P 2.62
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ERMJNUMAJOINUJHJ2CBIJMIDWJOWYHNBTPU
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(A)6.146.13(B)6.246.36Misfit6.156.1
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(A)(B)(C)(D)▲▲Figure 10. The co
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Luo, Y., Y. Tan, S. Wei, D. Helmber
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−44˚00' −43˚00'4-Sep-2010Mw 7
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TABLE 1Pairs of SAR imagery used in
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Depth (km)Coulomb Stress Change(bar
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Crippen, R. E. (1992). Measurement
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AlpineFaultHope Fault38 mm/yr0+ +-1
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σ 1dσ 3Nuσ 3CM w 7.1dw 6.2u70°M
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Right-lateral Faults(A) Range Front
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DISCUSSIONThe 2010-2011 Canterbury
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Large Apparent Stresses from the Ca
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Fine-scale Relocation of Aftershock
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−43.25°OXZ0 10 20km−43.5°−4
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REFERENCESAvery, H. R., J. B. Berri
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▲ ▲ Figure 2. A) shows three-co
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0.8PRPC Z0.40Normalized (Max PGA +
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Near-source Strong Ground MotionsOb
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(A)Magnitude, M w876542009 NZdataba
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Scale0.5 g5 seconds▲▲Figure 4.
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(A)(B)Spectral Acc, Sa (g)North/Wes
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Vertical-to-horizontal PGA ratio543
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REFERENCESAagaard, B. T., J. F. Hal
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Spectral Acceleration (0.3 s), (g)I
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Spectral Acceleration (3 s), (g)In[
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TABLE 1Mean (μ LLH ) and standard
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the small horizontal relative motio
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80°100°120°140°EXPLANATIONBorde
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Chang, K. H. (1997). Korean peninsu
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Wheeler, R. L. (2008). Paleoseismic
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A significant outcome of this study
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TABLE 1 (continued)Earthquakes for
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Meeting CalendarM E E T I N GC A L
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