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Jökull - 01.01.2015, Qupperneq 53

Jökull - 01.01.2015, Qupperneq 53
Seismicity beneath Þeistareykir, NE-Iceland Drouin et al., 2013, Metzger et al., 2013), but more recently explained by a combination of processes in- cluding plate spreading, viscoelastic relaxation, and inflation/deflation of shallow magma chambers be- neath Þeistareykir and Krafla (Ali et al., 2014). The base of the fault locking zone, sometimes equated with the seismogenic zone within which interseismic strain accumulates (Smith-Konter et al., 2011), is es- timated from geodetic data to be at 5.1–9.5 km depth (Metzger et al., 2011; Ali et al., 2014). Using a short-term seismic network of six stations Vogfjörð (2001) located several microearthquakes along a N-S line beneath northern Bæjarfjall at less than 3 km depth. Most of the events originated at 0.5–2.1 km depth. An increase in seismicity at Þeistareykir in 2007–2010 (Hjaltadóttir and Vogfjörð, 2011), coincided temporally with the local geodetic uplift signal. Local magnitudes (ML) ranged from -0.6 to 3.2. Shallow earthquakes were found to mostly follow the geothermally altered surface manifesta- tions suggesting that active underlying faults facilitate the transfer of geothermal fluids. Exploration wells have been used to build a hy- drothermal model of the upper 2.8 km in the past decade. Geothermal fluids beneath well ÞG-2 (Fig- ure 1b) originate from a deep (1600–1700 m depth) steam-dominated aquifer at ≥300◦C, where fluids propagate upwards along fractures and partly con- dense (Ármannsson, 2014). Beneath the vertical well ÞG-1, surface steam comes from a shallow (600– 700 m depth) water-dominated aquifer at 200–280◦C, which is fed in turn from the deeper steam-dominated aquifer. The deepest wells exhibit maximum geother- mal fluid temperatures of 380◦C (Sveinbjörnsdóttir et al., 2015) pointing towards an existing heat source within the upper crust. Transient electromagnetic (TEM) and magneto- telluric (MT) data inversions (Yu et al., 2008; Karls- dóttir et al., 2012) outline a low resistivity cap at 400– 800 m depth north of and slightly deeper beneath Bæj- arfjall. Low resistivity caps overlying high resistivity cores are characteristic structures in high-temperature geothermal systems in Iceland correlating well with the dominant alteration minerals of low and high tem- perature systems, respectively (Árnason et al., 2008). Thus, the TEM/MT results appear to coincide well with the hydrothermal model based on well informa- tion. Two distinct low-resistivity anomalies are found in the southeastern part of Bæjarfjall at 5–6 km depth b.s.l. and northeast of Bæjarfjall (beneath Ketilfjall) at 2.5–12 km depth b.s.l. and are interpreted as up- flow zones of heat into the geothermal systems above (Karlsdóttir et al., 2012). Petrological analyses of erupted lava (Borgar- hraun flow) suggest that crystallization of basalts oc- curred over a range of depths beneath Þeistareykir, where primitive basalts started crystallizing at the base of the crust (20–30 km depth) or uppermost man- tle and more evolved basalts formed in the shallow- mid crust (Maclennan 2008; Winpenny and Maclen- nan, 2014). SEISMIC DATA PROCESSING AND RESULTS A temporary seismic array of up to 31 three- component seismometers recorded the seismicity within the northern NVZ in the period August 2009 to July 2012. The array was operated by the University of Cambridge with additional stations from the IMO and covers the Krafla and Þeistareykir geothermal sys- tems (Figures 1a and 2c). A coalescence microseis- mic mapping algorithm (Drew et al., 2013) was used for automated event detection, where a short- to long- term average onset function is continuously computed from the horizontal and vertical amplitude compo- nents. The magnitudes are then back-migrated into the subsurface forming ‘coalescence’ functions with peak values indicating likely hypocenter locations and origin times. The Krafla starting model (Schuler et al., 2015) was used to estimate the travel times and ini- tial hypocenter localizations. Of the 5338 identified earthquakes within the Þeistareykir area, we removed events that had an average signal-to-noise ratio < 2.5 at a minimum of five stations. P- and S-wave arrivals times of 199 events were then manually repicked and picking errors (0.01 s, 0.02 s, 0.05 s, 0.1 s, or 0.2 s) assigned to each by visually inspecting the change in amplitude exceeding the background noise as well as change of signal frequency. JÖKULL No. 65, 2015 53
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