Jökull


Jökull - 01.01.2011, Page 36

Jökull - 01.01.2011, Page 36
J. Tarasewicz et al. ond, we consider the effect of using different velocity models to invert arrival time data. Variation in network geometry It is well established that, in order to place good con- straints on earthquake hypocentres, a network ide- ally needs to have both good azimuthal coverage of the source and one or more stations close to the epi- centre (e.g., Bondár et al., 2004; Bai et al., 2006; Martens et al., 2010). Proximal stations are espe- cially important for constraining the depth of earth- quake sources. For ice-capped volcanoes such as Eyjafjallajökull, seismicity occurring directly beneath the glacier is rarely recorded by such an ideal network configuration, given the difficulties of seismic moni- toring on glaciers. Seismicity in Iceland is routinely monitored by the Icelandic Meteorological Office (IMO), which oper- ates a permanent national network of seismometers. In early March 2010, the IMO network included three stations within 15 km of Eyjafjallajökull and another four within 50 km. Two weeks prior to the initial fis- sure eruption, the Institute of Earth Sciences, Univer- sity of Iceland deployed an additional six seismome- ter stations around the base of Eyjafjallajökull (Figure 1). These temporary stations were all within 4–15 km of the epicentres of the main seismic activity during early–mid March 2010. Data from the more proximal temporary stations were combined with data from the IMO stations to obtain the hypocentre locations re- ported by Tarasewicz et al. (in press). Variation in assumed velocity model The velocity structure beneath Eyjafjallajökull has not been constrained directly by tomographic studies or refraction profiles that transect the edifice. Based on data from other similar volcanoes, Eyjafjallajökull is likely to have marked lateral variation in velocity structure, at least at shallow levels. There is there- fore uncertainty regarding what velocity structure it is most appropriate to assume in calculating hypocen- tral locations. Tarasewicz et al. (in press) use a 1- D velocity model (VM1, see Figure 2e) based on the eastern end of the SIST refraction profile (Bjarnason et al., 1993) and the northern part of the Katla refrac- tion profile (Gudmundsson et al., 1994). The SIST profile crossed the South Iceland Seismic Zone, with its easternmost shotpoint in the Gígjökull lake, at the central-northern margin of Eyjafjallajökull. The Katla profile lay NNW-SSE across Mýrdalsjökull, crossing the western Katla caldera. Both of these profiles re- port similar velocity gradients and increased upper crustal thickness in the vicinity of Eyjafjallajökull. A marked increase in upper crustal thickness is observed going east across the South-Iceland Seismic Zone into the Eastern Volcanic Zone (EVZ) (Bjarnason et al., 1993; Pálmason, 1971). The depth below sea level to the 5.0 km/s isovelocity surface, which is a proxy for depth to the base of extrusive volcanics, is ∼2 km within the southern propagating tip of the EVZ. The depth to the 6.5 km/s isovelocity surface ranges from 5–10 km around Eyjafjallajökull (Brandsdóttir and Menke, 2008). The IMO use an alternative velocity model (VM2, Figure 2e) with slightly thinner upper- most crust and thus higher velocities in the 3–6 km depth range (Vogfjörð et al., 2002). Both velocity models use a Vp/Vs ratio of 1.77 in the upper crust. EARTHQUAKE DATA We have used five earthquakes with local moment magnitudes (Mlw) greater than 2.5 (Table 1) as a sam- ple to test the effects of varying the hypocentral lo- cation inversion parameters. All occurred under the northeastern flank of Eyjafjallajökull during March 2010 and all have hypocentres within the region of in- tense seismicity that occurred in the two weeks lead- ing up to the Fimmvörðuháls eruption (Figure 2). The test events were some of the largest-magnitude earth- quakes to occur around Eyjafjallajökull during March 2010 and all display clear P- and S-wave arrivals at all stations in the network that were operating at the time (Figure 3). This means that arrival time picks of the P-wave and S-waves are unambiguous. As such, these test events are both some of the best-constrained ex- amples and are also representative of the several thou- sand other earthquakes that are found to be co-located within a consistent depth range, when a consistent set of location inversion parameters is employed. We first use a Coalescence Microseismic Mapping (CMM) technique (Drew, 2010; Brandsdóttir et al., 2010; Tarasewicz et al., in press) to find hypocen- 36 JÖKULL No. 61, 2011
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