Jökull


Jökull - 01.01.2010, Page 27

Jökull - 01.01.2010, Page 27
The 2008 South Iceland Seismic Zone aftershock sequence posterior probability for the time and location of an event. This has been verified experimentally (Drew et al., 2005; Drew, 2010). For this data, an STA/LTA ra- tio of 0.1/ 0.4 s was used to detect P phases and 0.2/0.6 s to detect SH phases. Table 1. LOKI stations deployment overview. – Uppsetning færanlegra jarðskjálftamæla. Station Name Deployment Station code GUFU 29/5/2008 21:46 9881 SOLV 29/5/2008 23:16 987A ORLH 30/5/2008 00:30 988B HEIDI 30/5/2008 01:13 9870 HOLL 30/5/2008 03:10 987B RAUH 30/5/2008 18:00 9886 RANI 30/5/2008 19:00 9879 HOLT 30/5/2008 21:02 987C HALS 30/5/2008 22:34 A01A BURF 31/5/2008 16:53 A06F VNES 31/5/2008 19:02 A06E UGAR 21/6/2008 16:31 986F The program exists in two forms, CMM Detect and CMM Locate. Both programs make use of a Look Up Table (LUT) of modelled travel times from each station to every cell of a specified grid (i.e. a search area). CMM Detect performs a systematic exhaustive search over the grid, with candidate events identified as the time and location that the coalescence function exceeds a pre-set threshold (Figure 3). CMM Locate takes a list of event times, and evaluates the objective function over short time windows, returning an up- dated estimate of the time and location for each event. This is much quicker and easier than re-running CMM Detect, allowing the effects of changes to input pa- rameters to be quickly tested. A cell size of 320 m3 was used for most of the runs, then reduced to 230 m3 for the final run of CMM Locate. Using smaller cells is computationally more costly, without necessarily resulting in any real gains in accuracy. The optimal spatial sampling is governed by the shape (smoothness) of the mapped objective function, which is in turn governed by the input data (the constraints on arrival times) and the misfit be- tween data and model (residual). The time corresponding to the local maximum of the STA/LTA signal, will be shifted in time with re- spect to an interactive arrival time pick. As long as the shift in time is consistent between the time picks for each of the phase arrivals, the result is a shift in the estimated time of the event, not the estimated lo- cation. As the CMM program exhaustively evaluates for all times, it will also evaluate a second peak of emergent P energy arrivals. However, as long as the signal-to-noise ratio of the primary arrival is bigger, and the primary arrival fits the modelled traveltime equally well, the CMM estimated time and location will correspond to the primary arrival. Figure 3. Cartoon showing coalescence of signals from three stations. The dashed lines mark equal ray travel time from each of the stations. As they are migrated back towards their respective stations, they eventually intersect at the event location. Fig- ures from Drew (2010). – CMM forritið skynjar og staðsetur jarðskjálfta með því að nema útslag og bera saman reiknaðan ferðatíma til hverrar stöðvar. Utilizing a cluster, with each day of data processed as a separate run, the time required to processes the dataset was between 24 and 36 hours. In each run the data was band-pass filtered 2–12 Hz for S waves and 4–20 Hz for P waves. JÖKULL No. 60 27
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