Jökull


Jökull - 01.12.1976, Blaðsíða 14

Jökull - 01.12.1976, Blaðsíða 14
the blasts it is possible to calculate the thickness of layer 0. This thickness was found not to be significantly different from Pálmason’s results on the profile east of Hekla. A significant dif- ference was found, however, for the thickness of layer 1. Since apparent velocity correspond- ing to the velocity in layer 1 was measured across the array the cross-over distance between the head wave arrivals from layer 1 and layer 2 must be greater than 12 km. Thus a lower limit of 2.0 km is found for the thickness of layer 1. As described earlier the crustal velocity model in Table 1 was approximated by a model with layers of constant velocity gradients. The latter model was then used as an input for the loca- tion program. Using the location program to locate the ex- plosions it was found that the distances and depths were well within the error limits, but the azimuths were systematically wrong by 15— 18°. This systematic deviation can be corrected by assuming a time delay of 0.05 sec on the southeasternmost station in the array. A dip of the interface between layer 0 and layer 1 of 10° to the SE would cause the necessary time delay. Many different combinations of relative time delays can produce the observed error in azi- muth. But since the apparent velocity of the explosions NE of the array was not significantly in error the azimuth error is most likely caused by a time delay on the south-easternmost sta- tion. Furthermore it can be explained by a dipping interface with a strike parallel to the structural grain of the region. Fortunately most of the earthquakes occurred close to the lake where the explosions were made. Thus the azimuth corrections applied to most of the earthquakes were nearly identical to those applied to the explosions and are therefore independent of any assumptions about irregularities in the crustal structure. During the period of seismic recording at Hekla a swarm of earthquakes occurred near Sandvatn about 50 km to the NNW of Hekla (Fig. 1). Numerous earthquakes of that swarm were recorded by the Hekla array. Judging from the crustal structure, the distance and the probable depth of these earthquakes the first P-wave should arrive at the Hekla array with an apparent velocity of about 6.5 km/sec, which is the P-velocity in layer 3. It was found, how- 12 JÖKULL26. ÁR ever, that the apparent velocities were signi- ficantly lower, averaging about 5.5 km/sec. As before it is possible to explain this difference by assuming a time delay on tlie southeastern- most station. The necessary delay is of the same magnitude as the one necessary to explain the discrepancy in tlie azimuth of the explosions. If interpreted in terms of dipping layers this observation implies that all interfaces down to and including the layer 2 — layer 3 interface have the same dip of 10° to the SE. THE SEISMIC ACTIVITY Before the eruption An examination of the records from the WWNSS seismograph station at Akureyri and the Preliminary Seismograph Readings of the Meteorological Office do not reveal any un- usual seismic activity around Hekla during several weeks prior to the eruption. Two earth- quakes of magnitudes 2.8 and 3.3 were recorded on April 16 and 18 respectively with epicenters possibly near Hekla. These events would by no means awaken any suspicion of an impending eruption. It is possible, however, that significant activity occurred but was too weak to be re- corded by the permanent seismic stations. A considerable number of weak earthquakes oc- curred prior to the 1973 Heimaey eruption (Fig. 1) and was recorded by two short-period seismometers located at the distances of 60 and 90 km (Björnsson and Einarsson, paper in pre- paration). This activity was not observed by the permanent seismic network. The beginning of the eruption During the last half hour before the start of the eruption, earth tremors were recorded by all three permanent seismic stations in Iceland. These tremors were continuous and their ampli- tude increased steadily until 21:18 when there was a sudden burst of tremors (Fig. 3). After that time numerous bursts occurred superim- posed on the continuous tremors. These bursts are probably S-waves and surface waves of earthquakes. For some of them the correspond- ing P-waves could be found on the records with S-P time appropriate for earthquakes near Hekla. These events were of magnitudes be- tween 3.6 and 4.0. No particularly outstanding
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