Jökull


Jökull - 01.01.2010, Side 114

Jökull - 01.01.2010, Side 114
Hjartardóttir et al. the stress field would be governed by the differential movements caused by the deglaciation. The Kerling- ar fault displays characteristics which may indicate that the fault was formed without the involvement of magma; it is long (∼30 km) and continuous, as op- posed to the sinuous and discontinuous normal faults characteristic of dike-induced rifts. This indicates that the stress field causing the formation of the Kerlingar fault extended over a large area. We consider it likely that numerous other faults at the boundary between the NVZ and the EFB formed in a similar manner, and that magma intruded some of them, either verti- cally from the mantle, or horizontally from the Kverk- fjöll central volcano. This process could have formed the distinct arcuate pattern of hyaloclastite ridges seen at the boundary between the NVZ and the EFB, in the continuation of the Kverkfjöll fissure swarm (Fig- ure 1). Differential movements, as suggested here, would have been confined to this area and not applicable to other flank zones of the Icelandic rift. In par- ticular, this does not apply to the southernmost part of the NVZ-EFB boundary, as no marked difference in crustal thickness exists there (e.g. Allen et al. 2002; Brandsdóttir and Menke 2008; Darbyshire et al. 1998). Variations in crustal thickness along the margin of the NVZ could also explain why the dis- tinct arcuate pattern of hyaloclastite ridges seen at the NVZ-EFB boundary does not extend all the way to the Kverkfjöll central volcano (Figure 1). It has been proposed that stress changes during deglaciations have caused the formation of faults in continental settings, such as in Fennoscandia (e.g. Muir Wood 1989). These are thrust faults, consistent with horizontal compression in the old, continental crust (Sykes and Sbar 1974; Wu et al. 1999). How- ever, the reaction of the NVZ-EFB crust to deloading should be different. Crustal extension is expected in the much younger crust (Árnadóttir et al. 2009; Sykes and Sbar 1974). In this paper, we have presented an overview on the processes that may cause differential movements at the NVZ-EFB boundary. For a more detailed study, modeling of these deloading effects (i.e. with Finite Element Modelling) is preferable. CONCLUSIONS 1. The Kerlingar fault is a 30 km long normal fault located on the eastern boundary of the Northern Vol- canic Rift Zone, Iceland. It is a gently curved NNW- oriented feature. The fault is located within and par- allel with hyaloclastite ridges which form an arcuate pattern along the boundary of the NVZ and the EFB. 2. The fault has some notable features: a. It is un- usually long and continuous, compared with fractures and normal faults within the NVZ. b. It has a throw down to the east, although it is located at the eastern boundary of the NVZ. c. It is not parallel with the fis- sure swarms in the NVZ at this latitude, although it is parallel with hyaloclastite ridges at the NVZ-EFB boundary, as well as with several other faults at the same boundary. 3. Although no earthquakes have been instrumen- tally detected in the area, the sharpness and continu- ity of the fault indicate that it has been active in the Holocene. The fault has most likely been active in many earthquakes but assuming it ruptured in only one event, its magnitude would have been close to Mw=6.7. 4. The offset of fault segments we observed in the field was in the range 2–9 m. The higher number might be an overestimate because of erosion due to snow melting. 5. We found a sharp offset in a moraine formation in a part of the Kerlingar fault, which shows that the fault has been active since the Pleistocene glacier dis- appeared from the area. 6. Considering three possible explanations for the formation of the Kerlingar fault, we conclude that the most likely process is differential movements due to deglaciation, isostatic rebound and variations in crustal buoancy. Lower viscosity of the lower crust and uppermost mantle induces faster rebound within the NVZ and buoyancy generates higher uplift of the NVZ than the adjacent EFB, explaining why the Kerl- ingar fault is situated at the NVZ-EFB boundary, why it is parallel with the boundary, and why it is so long and continuous. Other faults on the NVZ-EFB bound- ary may be formed in a similar manner. Magma may have intruded some of them, forming the arcuate pat- tern of hyaloclastite ridges at the NVZ-EFB boundary. 114 JÖKULL No. 60
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