(A)(A)(B)(B)▲▲Figure 10. Comparison of CSR M7.5 for the Darfield andChristchurch earthquakes with CRR M7.5 for a site in Bexley(FC = 9%): A) profiles for DCP test; and B) profiles for SASWtest.In general, the selected critical layer thickness was thinnest forcases of lateral spreading with no ejecta, intermediate for lateralspreading with ejecta, and thickest for large sand boils withno associated lateral spreading. For example, the profile shownin Figure 10A laterally spread (see Figure 4) and there was asignificant amount of ejecta that vented to the ground surfacenearby. Using this information, and trends in the N DCPT ,shown in Figure 5B, the selected critical layer was ~2 m thick,as indicated in Figure 10A. Once the critical layers were determinedfor each test site, the N 1,60cs-SPTequiv values, CSR M7.5 ,and CRR M7.5 were averaged over these depths. The results wereplotted along with Youd et al. (2001) SPT CRR M7.5 curve inFigure 11A.A similar procedure as that outlined above was used tocompute the CSR M7.5 for the SASW test sites. However, theMSF proposed by Andrus and Stokoe (2000) was used instead▲ ▲ Figure 11. Comparison of predicted versus observed liquefaction:A) DCP test; and B) SASW test.of the average of the recommended range proposed by Youdet al. (2001). The reason for using slightly different MSFs wasto be consistent with how the respective cyclic resistance ratiocurves were developed from the observational data. Usingthe computed V S1 , the CRR M7.5 for the test site profiles werecalculated following the Andrus and Stokoe (2000) procedure;this procedure is also outlined in Youd et al. (2001).Comparisons of the computed CSR M7.5 for both the Darfieldand Christchurch earthquakes and CRR M7.5 for a test site inthe eastern Christchurch suburb of Bexley are shown in Figure10B. Consistent with the DCP test results, liquefaction ispredicted to occur at this site during both the Darfield andChristchurch earthquakes, with the liquefaction predicted tobe more severe during the Christchurch earthquake. Again,these predictions are in line with the post-earthquake observations.936 Seismological Research Letters Volume 82, Number 6 November/December 2011
Using the same critical layers as selected for DCP testliquefaction evaluations, V S1 , CSR M7.5 , and CRR M7.5 wereaveraged over the critical depths for each test site profile. Theresults were plotted along with the Andrus and Stokoe (2000)CRR M7.5 curves in Figure 11B.DISCUSSIONAs shown in Figure 11, the liquefaction predictions made usingboth the DCP and SASW test data reasonably match fieldobservations. This is particularly significant for the DCP databecause a correlation was first required to convert the measuredN DCPT to SPT N-values (shown in Figure 5A), and undoubtedly,this correlation is inherently uncertain. Also, the DCPwas only able to test down to a depth of ~6 m at a maximumand usually less than about 4.5 m. Below this depth, N DCPTbecame large because of the presence of a dense layer and/orbecause of the increase in effective confining stress. Becausethe DCP is manually operated, performing tests beyond ~5 mdepths becomes very laborious even in relatively loose sanddeposits. The SASW test was able to test to deeper depths thatthe DCP, but was still limited to depths of ~6 to 9 m with thesledge hammer source. These depth limits are true shortcomingsof both tests because at a few DCP and SASW test sites,available cone penetration test (CPT) soundings indicated thepresence of potentially liquefiable layers deeper in the profiles.As a result, our selected critical layer may only be one of multiplecritical layers in the profile and may not be the most critical.Also from Figure 11, it can be noted that most of the DCPand SASW tests were performed at sites that liquefied, with apaucity of data from sites that did not liquefy. The reason forthis is the manifestation of liquefaction at the ground surfaceis a definite indication that liquefiable soils are present. Severalno-liquefaction sites were investigated, especially ones adjacentto sites that liquefied. However, in the majority of these caseswe were not able to find a sandy stratum below the groundwater table in the upper ~5 m of these sites using the handauger.As a result, DCP tests were not performed at these sites,and the sites were not included in the DCP database.CONCLUSIONSThe U.S. and New Zealand members of the GEER team performedDCP and SASW tests after the 4 September 2010 M w7.1 Darfield earthquake and the 22 February 2011 M w 6.2Christchurch earthquake. Both tests are relatively portable,making them suitable for rapid, post-earthquake investigations.Of particular interest to the team were characterizing sites thatliquefied during either one or both of the earthquakes. Usingthe in-situ test data in combination with estimated PGAs,the liquefaction potential at the test sites was evaluated andcompared with post-earthquake observations. Despite someshortcomings of the tests, they did a relatively good job in correctlypredicting the occurrence/non-occurrence of liquefaction,proving the value of these tests for rapid, post-earthquakeinvestigations.ACKNOWLEDGMENTSThe primary support for the US GEER Team memberswas provided by grants from the U.S. National ScienceFoundation (NSF) as part of the Geotechnical Extreme EventReconnaissance (GEER) Association activity through CMMI-00323914 and NSF RAPID grant CMMI-1137977. Also,Dr. Wotherspoon’s position at the University of Aucklandis funded by the Earthquake Commission (EQC). However,any opinions, findings, and conclusions or recommendationsexpressed in this material are those of the authors and do notnecessarily reflect the views of the National Science Foundationor the EQC.REFERENCESAbrahamson, N. A. and R. R. Youngs (1992). A stable algorithm forregression analyses using the random effects model. Bulletin of theSeismological Society of America 82 (1), 505–510.Allen, J., S. Ashford, E. Bowman, B. Bradley, B. Cox, M. Cubrinovski,R. Green, T. Hutchinson, E. Kavazanjian, R. Orense, M. Pender,M. Quigley, and L. Wotherspoon (2010a). Geotechnical reconnaissanceof the 2010 Darfield (Canterbury) earthquake. Bulletin of theNew Zealand Society for Earthquake Engineering 43 (4), 243–320.Allen, J., S. Ashford, E. Bowman, B. Bradley, B. Cox, M. Cubrinovski, R.Green, T. Hutchinson, E. Kavazanjian, R. Orense, M. Pender, M.Quigley, and L. Wotherspoon (2010b). Geotechnical Reconnaissanceof the 2010 Darfield (New Zealand) Earthquake. GEER AssociationReport No. GEER-024, ed. R. A. Green and M. Cubrinovski.Andrus, R. D., and K. H. Stokoe II (2000). Liquefaction resistance ofsoils from shear wave velocity. ASCE Journal of Geotechnical &Geoenvironmental Engineering 126 (11), 1,015–1,025.Bradley, B. A. (2010). NZ-specific Pseudo-spectral Acceleration GroundMotion Prediction Equations Based on Foreign Models. Departmentof Civil and Natural Resources Engineering, University ofCanterbury, Christchurch, New Zealand, 324 pp.Brown L. J., R. D. Beetham, B. R. Paterson, and J. H. Weeber (1995).Geology of Christchurch, New Zealand. Environmental &Engineering Geoscience 1 (4), 427–488.Cox, B. R., and C. M. Wood (2010). A comparison of linear-array surfacewave methods at a soft soil site in the Mississippi Embayment. InGeoFlorida 2010: Advances in Analysis, Modeling, and Design, ed.D. O. Fratta et al., 1,369–1,378. Reston, VA: American Society ofCivil Engineers.Cox, B. R., and C. M. Wood (2011). Surface wave benchmarking exercise:Methodologies, results and uncertainties. In GeoRisk 2011:Geotechnical Risk Assessment and Management, ed. C. H. Juang etal., 845–852. Reston, VA: American Society of Civil Engineers.Cubrinovski, M., J. D. Bray, M. Taylor, S. Giorgini, B. Bradley, L.Wotherspoon, and J. Zupan (2011). Soil liquefaction effects in thecentral business district during the February 2011 Christchurchearthquake. Seismological Research Letters 82, 893–904.Environment Canterbury (ECan) (2004). Solid Facts on ChristchurchLiquefaction. Environment Canterbury, Christchurch, NewZealand; http://ecan.govt.nz/publications/General/solid-factschristchurch-liquefaction.pdf.Gerstenberger, M., M. Cubrinovski, G. McVerry, M. Stirling, D.Rhoades, B. Bradley, R. Langridge, T. Webb, B. Peng, J. Pettinga,K. Berryman, and H. Brackley (2011). Probabilistic Assessment ofLiquefaction Potential for Christchurch in the Next 50 Years. GNSScience Report 2011/15, 30 pp.Goda, K., and H. P. Hong (2008). Spatial correlation of peak groundmotions and response spectra. Bulletin of the Seismological Societyof America 98 (1), 354–465.Seismological Research Letters Volume 82, Number 6 November/December 2011 937
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Volume 82, Number 6 November/Decemb
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News and Notes (continued)Nominatio
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Preface to the Focused Issue on the
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TABLE 1Peak ground acceleration (PG
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▲▲Figure 2. A) Sketch of the
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▲▲Figure 4. A) Adopted moment r
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▲▲Figure 7. As in Figure 6 but
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▲ ▲ Figure 8. Misfit parameters
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▲ ▲ Figure 10. Spatial variabil
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▲ ▲ Figure 12. Standard spectra
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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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▲▲Figure 4. Convergence of inve
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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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(A)(B)(C)(D)▲▲Figure 12. 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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10Obs SA(1s)AS1AS+SDAB 2006AB+SDSA(
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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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A’0 km 4 8−43.5°B’B−43.6°
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REFERENCESAvery, H. R., J. B. Berri
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▲ ▲ Figure 2. A) shows three-co
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▲ ▲ Figure 4. Vertical accelera
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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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(A)(B)Station:CCCCSolid:AvgHorizDas
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REFERENCESAagaard, B. T., J. F. Hal
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▲ ▲ Figure 1. Shear-wave veloci
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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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Strong Ground Motions and Damage Co
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ings and the Modified Takeda-Slip M
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high, but there were no buildings d
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REFERENCES▲▲Figure 8. Heavily d
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(A)(B)(C)(D)(E)▲▲Figure 1. A) M
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TABLE 1 (continued)Earthquakes for
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▲▲Figure 2. Earthquakes used in
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Meeting CalendarM E E T I N GC A L
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201 Plaza Professional Bldg. • El
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Seismological Research Letters (SRL
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Christa von Hillebrandt-Andrade, Pr