▲ ▲ Figure 2. Distribution of fault slip inferred in the 22 February 2011 Christchurch earthquake (Beavan et al. 2011, this issue). Arrowsindicate the slip vector. The inferred hypocenter is indicated by a star.issue). It can be seen that slip on the fault occurred obliquelywith both significant up-dip and along-strike components(average rake, λ = 146°). The steeply dipping nature of the fault(δ = 69°), as well as the large up-dip component of slip, contributedto the large observed vertical accelerations discussed inthe next section. For the purpose of the subsequent engineeringanalysis of strong ground motion, the Beavan et al. (2011, page789 of this issue) finite fault model was “trimmed” using themethodology of Somerville et al. (1999), which resulted in theremoval of 1 km from the northeast and southwest extents ofFigure 2. The resulting “trimmed” fault therefore has dimensionsof 15 km along-strike and 8 km down-dip, giving a totalarea of 120 km 2 .Christchurch is located on the Canterbury Plains, a fandeposit resulting from the numerous rivers flowing eastwardfrom the foothills of the Southern Alps (Brown and Weeber1992). In the vicinity of Christchurch, the Canterbury Plains arecomprised of a complex sequence of gravels interbedded with silt,clay, peat, and shelly sands. The fine sediments form aquicludesand aquitards between the gravel aquifers, and with the nearbycoastline to the east, result in the majority of Christchurch havinga water table less than 5 m depth, with the majority of thearea including, and to the east of, the central business districthaving a water table less than 1 m from the surface (Brown andWeeber 1992). The postglacial Christchurch Formation createdby estuarine, lagoonal, dune, and coastal swamp deposits (containinggravel, sand, silt, clay, shell, and peat) is the predominantsurface geology layer in the Christchurch area, which outcropsup to 11 km west of the coast and has a depth of approximately40 km along the coast itself (Brown and Weeber 1992). At thesoutheast edge of Christchurch lies the extinct Banks Peninsulavolcanic complex.STRONG MOTION RECORD PROCESSINGVolume 1 ground motion records were obtained from GeoNet(http://www.geonet.org.nz/) and processed on a record-byrecordbasis. The overall processing methodology adopted iselaborated in Chiou et al. (2008, Figure 4). All ground motionswere processed with a low-pass causal Butterworth filter of50 Hz, and while the corner frequency of the high-pass filterwas record-specific, a frequency of less than 0.05 Hz providedphysically realistic Fourier spectra amplitudes and integrateddisplacement histories for all the near-source ground motions.Owing to the digital nature of all of the instruments, baselinecorrections were found to be unnecessary following theabove filtering. As a result, the processed ground motions canbe considered to provide reliable estimates of peak groundaccelerations (PGA) and spectral ordinates over the range0.01–10 seconds (Douglas and Boore 2010), which are typicallyof engineering interest. It should be noted that the aboveprocedure does not lend itself to the computation of residualdisplacements, which may be non-zero for near-source locations.However, as a result of possible instrument tilting, whichmay be significant at sites where liquefaction occurred, reliablecomputation of such residual displacements may not be possible(Graizer 2005) and is left for future study.854 Seismological Research Letters Volume 82, Number 6 November/December 2011
(A)Magnitude, M w876542009 NZdatabase04/09/201022/02/201110 0 10 1 10 2Distance, R rup(km)(B)Number of exceedances2009 NZdatabase04/09/201022/02/2011Total10 110 00.2 0.4 0.6 0.8 1 1.2 1.4102Peak ground acceleration, PGA (g)▲ ▲ Figure 3. Significance of the 22 February 2011 Christchurch and 4 September 2010 Darfield earthquakes in relation to previouslyrecorded ground motions in New Zealand: A) magnitude-distance distribution; B) exceeded values of peak ground acceleration.While New Zealand can be considered as a region of highseismicity in a global context, prior to the 4 September 2010Darfield and 22 February 2011 Christchurch earthquakesthere was a paucity of high-amplitude recorded strong groundmotions, primarily as a result of a sparse instrumentation networkbefore the commencement of GeoNet in 2001. Figure3 illustrates the magnitude-distance distribution of recordedground motions from active shallow crustal earthquakes up to2009 as complied by Zhao and Gerstenberger (2010). Also illustratedin Figure 3A are the ground motions recorded in both the4 September 2010 Darfield and 22 February 2011 Christchurchearthquakes. The significance of the recorded ground motionsin these two earthquakes is even more apparent if the groundmotions in Figure 3A are plotted in terms of their geometricmean horizontal PGA. Figure 3B illustrates the number ofground motions exceeding specific values of PGA. It can beseen that up to 2009, the maximum PGA recorded in NewZealand was 0.39 g, with only seven observed ground motionsexceeding 0.2 g PGA. Figure 3B also illustrates the exceedancevalues observed in the Darfield and Christchurch earthquakes.With the addition of these two events (not to mention recordsobtained from numerous significant aftershocks, which arenot discussed herein) it can be seen that ground motions of upto 1.41 g have now been recorded, with 12 observed groundmotions exceeding 0.4 g and 39 exceeding 0.2 g.OBSERVED NEAR-SOURCE GROUND MOTIONSTable 1 presents a summary of the ground motions in the widerChristchurch region that were recorded within a source-to-sitedistance of R rup = 20 km, including: station site class accordingto the New Zealand loading standard, New Zealand Standards1170.5 (2004); PGA, peak ground velocity (PGV); 5–95%significant duration, (D s5–95 ) (Bommer and Martinez-Pereira1999) for geometric mean horizontal component; and peakvertical ground acceleration (PGA v ).Figures 4–6 illustrate the spatial distribution of accelerationtime histories recorded at the aforementioned strongmotion stations in the form of fault-normal, fault-parallel,and vertical components, respectively. The aforementioned“trimmed” finite fault model of Beavan et al. (2011, page 789of this issue) is also shown. The following sections discuss variousaspects of the ground motions observed in Figures 4–6.Ground Motion on Rock and Soil SitesIn interpreting the observed ground motions in Figures 4–6, itis first worth noting that only the Lyttelton Port (LPCC) stationto the southeast of Christchurch is located on engineeringbedrock (i.e., site class B). Stations HVSC and LPOC locatednear the edge of the Port Hills rock outcrop are site class C,while all remaining stations are situated on the Christchurchsedimentary basin and are predominantly site class D (theexceptions being HPSC, NNBS, PRPC, and KPOC, which aresite class E). Unfortunately at present the site characterizationof strong motion stations in the Christchurch region, and NewZealand in general, is relatively poor with the above site classesdetermined from geological maps and direct surface inspection(N. Perrin, personal communication 2011), and details suchas P- and S-wave velocity, SPT, and CPT data not available.Clearly, obtaining such information is necessary for a rigorousanalysis of the observed ground motions, and is the focus ofimmediate studies. Nonetheless, a wealth of insight can still beobtained from inspection and analysis of the observed groundmotions.A direct comparison of the effect of soil and rock site canbe made by comparing the ground motions observed at LPCCand LPOC located at Lyttelton Port approximately 1 km apart.The LPCC instrument is located on engineering bedrock, andwhile detailed information of the site conditions at LPOC arepresently unavailable, it is said to be a relatively thin (~30 m)colluvium layer comprised primarily of silt and clay (J. Berrill,personal communication 2011). In addition to a comparison ofSeismological Research Letters Volume 82, Number 6 November/December 2011 855
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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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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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Comparison of Liquefaction Features
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(A)(B)▲▲Figure 2. A) Simplified
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(A)Acceleration (Gal)6004002000-200
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(A)(B)▲▲Figure 7. Distribution
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(A)(B)▲▲Figure 10. Damage to a
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(A)(B)▲ ▲ Figure 14. A) Subside
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Use of DCP and SASW Tests to Evalua
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each of the Waimakariri River and a
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▲ ▲ Figure 2. Horizontal peak g
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only minor damage, mostly to their
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(A)(C)(B)▲▲Figure 5. Ferrymead
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Events Reconnaissance (GEER) Associ
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New PublicationsCanGeoRefThe Americ
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Wednesday, 18 AprilTechnical Sessio
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Verification of a Spectral-Element
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EASTERN SECTIONRESEARCH LETTERSReas
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(A)70°N100°W 60°W70°N(B)100°E1
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Mongolia SCRThe presence or absence
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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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▲▲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