An entry from Ruth Gardner's blog for 21 April 2011 entitled, "Guarding the Graves".
A large patch of liquefaction amongst graves and tombstones in a cemetery in Christchurch.
A large patch of liquefaction amongst graves and tombstones in a cemetery in Christchurch.
A large patch of liquefaction amongst graves and tombstones in a cemetery in Christchurch.
Photograph captioned by BeckerFraserPhotos, "Damage to graves and tombstones in the Lyttelton Cemetery".
Photograph captioned by BeckerFraserPhotos, "Damage to graves and tombstones in the Lyttelton Cemetery".
Photograph captioned by BeckerFraserPhotos, "Damage to graves and tombstones in the Lyttelton Cemetery".
Photograph captioned by BeckerFraserPhotos, "Damage to graves and tombstones in the Lyttelton Cemetery".
Photograph captioned by BeckerFraserPhotos, "Damage to graves and tombstones in the Lyttelton Cemetery".
Broken head-stones as a result of the magnitude 6.3 quake in Christchurch - 22 February 2011. HDR process to add the "feeling" I felt at seeing this sort of damage.
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One landscape colour digital photograph taken on 30 June 2011 showing earthquake damage to graves in Lyttelton Roman Catholic and Dissenters (Public) Cemeteries in Reserve Terrace. Most of the headstones and grave surrounds in the photograph show damage. Looking east in the Dissenters (Public) section of the cemetery. The Lyttelton cemeteries a...
The Chief Coroner says the remains of 12 victims of the Christchurch earthquake may never be identified.
A digitally manipulated image of a fallen headstone. The photographer comments, "Since the September 2010 earthquake in Christchurch, New Zealand a lot of the headstones have fallen, but sadly a lot have not been resurrected to their former places".
In the days after the devastating earthquake on 22 February 2011, we lost water in my neighbourhood. However, I was able to supplement the water in our emergency kit with water from this spigot in Somerfield Cemetary. Thank you, William Russell.
This paper investigates the effects of variability in source rupture parameters on site-specific physics-based simulated ground motions, ascertained through the systematic analysis of ground motion intensity measures. As a preliminary study, we consider simulations of the 22 February 2011 Christchurch earthquake using the Graves and Pitarka (2015) methodology. The effects of source variability are considered via a sensitivity study in which parameters (hypocentre location, earthquake magnitude, average rupture velocity, fault geometry and the Brune stress parameter) are individually varied by one standard deviation. The sensitivity of simulated ground motion intensity measures are subsequently compared against observational data. The preliminary results from this study indicate that uncertainty in the stress parameter and the rupture velocity have the most significant effect on the high frequency amplitudes. Conversely, magnitude uncertainty was found to be most influential on the spectral acceleration amplitudes at low frequencies. Further work is required to extend this preliminary study to exhaustively consider more events and to include parameter covariance. The ultimate results of this research will assist in the validation of the overall simulation method’s accuracy in capturing various rupture parameters, which is essential for the use of simulated ground motion models in probabilistic seismic hazard analysis.
A photograph submitted by Sarndra to the QuakeStories website. The description reads, "Lyttelton Cemetery, Reserve Terrace, Lyttelton. Damage obvious in several areas. Christchurch’s cemeteries have suffered widespread damage to plots and headstones since 4 September 2010. This photo was snapped 10 April 2011. My pioneering ancestors will be turning in their graves :,-(".
Fallen headstone due to September 4th earthquake: Mary Ann DONALDSON Died 20 April 1908 aged 68 years Occupation: domestic of Division Street Born: England [information from cemetery online database and listed as in same plot as below] In loving remembrance of James DONALDSON who departd this life June 10th 1904 aged 77 years "Thou shalt come t...
One portrait colour digital photograph taken on 1 March 2011 showing earthquake damage to the Dry Dock Pump House. Photograph taken from Dampiers Bay Pile Moorings showing the eastern end of the building and the Cassion. Engineer The brick pump house for the Lyttelton Graving or Dry Dock was damaged in the 22 February 2011 earthquake. Lyttelton...
One landscape colour digital photograph taken on 22 March 2011 showing the demolition of the Dry Dock Pump House. Photograph taken from Brittan Terrace looking east over the Inner Harbour. Engineer The brick pump house for the Lyttelton Graving or Dry Dock was damaged in the 22 February 2011 Earthquake. Lyttelton Port of Christchurch decided to...
One landscape colour digital photograph taken on 22 March 2011 showing the demolition of the Dry Dock Pump House. Photograph taken from Cyrus Williams Quay beside the Cattle Jetty showing the southern side of the building. Engineer The brick pump house for the Lyttelton Graving or Dry Dock was damaged in the 22 February 2011 Earthquake. Lyttelt...
Fallen headstone due to September 4th earthquake: Mary Ann DONALDSON Died 20 April 1908 aged 68 years Occupation: domestic of Division Street Born: England [information from cemetery online database and listed as in same plot as below] In loving remembrance of James DONALDSON who departd this life June 10th 1904 aged 77 years "Thou shalt come t...
In this paper, we perform hybrid broadband (0-10 Hz) ground motion simulations for the ten most significant events (Mw 4.7-7.1) in the 2010-2011 Canterbury earthquake sequence. Taking advantage of having repeated recordings at same stations, we validate our simulations using both recordings and an empirically-developed ground motion prediction equation (GMPE). The simulation clearly captures the sedimentary basin amplification and the rupture directivity effects. Quantitative comparisons of the simulations with both recordings and the GMPE, as well as analyses of the total residuals (indicating model bias) show that simulations perform better than the empirical GMPE, especially for long period. To scrutinize the ground motion variability, we partitioned the total residuals into different components. The total residual appears to be unbiased, and the use of a 3D velocity structure reduces the long period systematic bias particularly for stations located close to the Banks Peninsula volcanic area.
The chair of the inquiry in to the Earthquake Commission has grave concerns about the state of the housing stock in Christchurch due to EQC's failure to properly fix quake damage. It's just one of a raft of findings released by Dame Silvia Cartwright today, after a year and a half long inquiry that heard from hundreds of homeowners and key players. Conan Young has the story.
One landscape colour digital photograph taken on 30 June 2011 showing signs warning of the danger posed by unstable headstones in Lyttelton Roman Catholic and Dissenters (Public) Cemeteries in Reserve Terrace. Several toppled headstones and collapsed grave surrounds are visible in the photograph. Looking east from the main gate. The Lyttelton c...
1. Background and Objectives This poster presents results from ground motion simulations of small-to-moderate magnitude (3.5≤Mw≤5.0) earthquake events in the Canterbury, New Zealand region using the Graves and Pitarka (2010,2015) methodology. Subsequent investigation of systematic ground motion effects highlights the prediction bias in the simulations which are also benchmarked against empirical ground motion models (e.g. Bradley (2013)). In this study, 144 earthquake ruptures, modelled as point sources, are considered with 1924 quality-assured ground motions recorded across 45 strong motion stations throughout the Canterbury region, as shown in Figure 1. The majority of sources are Mw≥4.0 and have centroid depth (CD) 10km or shallower. Earthquake source descriptions were obtained from the GeoNet New Zealand earthquake catalogue. The ground motion simulations were performed within a computational domain of 140km x 120km x 46km with a finite difference grid spacing of 0.1km. The low-frequency (LF) simulations utilize the 3D Canterbury Velocity Model while the high-frequency (HF) simulations utilize a generic regional 1D velocity model. In the LF simulations, a minimum shear wave velocity of 500m/s is enforced, yielding a maximum frequency of 1.0Hz.
This paper presents the ongoing development of a new 3D seismic velocity model of Canterbury, New Zealand. The model explicitly represents the Canterbury sedimentary basin, and other significant geologic horizons, which are expected to have important implications on observed ground motions. The model utilizes numerous sources of data, including 3D regional tomography with a variable-depth inferred Moho, seismic reflection survey lines, geotechnical boreholes and well logs, spectral analysis of surface waves, and CPT logs which provide velocity constraints over their respective ranges of application. The model provides P- and S-wave velocity and density (i.e. Vp, Vs and p) over a grid of input points, and is presently being utilized in broadband ground motion simulations of the 2010-2011 Canterbury earthquakes. Comparison of simulated ground motions with those observed in the 2010-2011 Canterbury earthquakes will help provide a better understanding of the salient physical processes which characterized the unique set of strong ground motions recorded in this sequence of earthquake events.
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his poster presents the ongoing development of a 3D Canterbury seismic velocity model which will be used in physics-based hybrid broadband ground motion simulation of the 2010-2011 Canterbury earthquakes. Velocity models must sufficiently represent critical aspects of the crustal structure over multiple length scales which will influence the results of the simulations. As a result, numerous sources of data are utilized in order to provide adequate resolution where necessary. Figure 2: (a) Seismic reflection line showing P-wave velocities and significant geologic horizons (Barnes et al. 2011), and (b) Shear wave profiles at 10 locations (Stokoe et al. 2013). Figure 4: Cross sections of the current version of the Canterbury velocity model to depths of 10km as shown in Figure 1: (a) at a constant latitude value of -43.6˚, and (b) at a constant longitude value of 172.64˚. 3. Ground Surface and Geologic Horizon Models Figure 3: (a) Ground surface model derived from numerous available digital elevation models, and (b) Base of the Quaternary sediments derived from structural contours and seismic reflection line elevations. The Canterbury region has a unique and complex geology which likely has a significant impact on strong ground motions, in particular the deep and loose deposits of the Canterbury basin. The Canterbury basin has several implications on seismic wave phenomena such as long period ground motion amplification and wave guide effects. Using a realistic 3D seismic velocity model in physics-based ground motion simulation will implicitly account for such effects and the resultant simulated ground motions can be studied to gain a fundamental understanding of the salient ground motion phenomena which occurred during the Canterbury earthquakes, and the potential for repeat occurrences in the Canterbury region. Figure 1 shows the current model domain as a rectangular area between Lat=[-43.2˚,-44.0˚], and Lon=[171.5˚,173.0˚]. This essentially spans the area between the foot of the Southern Alps in the North West to Banks Peninsula in the East. Currently the model extends to a depth of 50km below sea level.
This study examines the performance of nonlinear total-stress wave-propagation site response analysis for modelling site effects in physics-based ground motion simulations of the 2010-2011 Canterbury, New Zealand earthquake sequence. This approach allows for explicit modeling of 3-dimensional ground motion phenomena at the regional scale, as well as detailed site effects and soil nonlinearity at the local scale. The approach is compared to a more commonly used empirical VS30 (30 m time-averaged shear wave velocity)-based method for computing site amplification as proposed by Graves and Pitarka (2010, 2015).