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Volcano geodesy and magma dynamics in Iceland - Acri-ST

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20E. Sturkell et al. / Journal of <strong>Volcano</strong>logy <strong>and</strong> Geothermal Research 150 (2006) 14–34AH66NM1GM2KL10 km16WB 93-99curve with a decay constant of 39 years (Sturkell etal., submitted for publication). The geodetic data havebeen modeled <strong>and</strong> <strong>in</strong>terpreted <strong>in</strong> terms of a s<strong>in</strong>gleMogi-type pressure source (Mogi, 1958) locatedclose to the centre of the ma<strong>in</strong> Askja caldera (Tryggvason,1989; Rymer <strong>and</strong> Tryggvason, 1993; Sturkell<strong>and</strong> Sigmundsson, 2000). All these authors placed thepo<strong>in</strong>t source at 1.5 to 3.5 km depth. This modelA4291 km66NA406A404DYNG10 kmFig. 5. A) A InSAR amplitude image which <strong>in</strong>cludes the outl<strong>in</strong>e ofthe Krafla fissure swarm (dotted l<strong>in</strong>e) the Krafla central volcano(solid white l<strong>in</strong>e), the caldera (white dashed l<strong>in</strong>e) <strong>and</strong> the location oftwo model sources, a shallow <strong>magma</strong> chamber (M2) <strong>and</strong> about 20km deep source (M1). The location of the area is given <strong>in</strong> Fig. 1. B)An <strong>in</strong>terferogram spann<strong>in</strong>g the period from 1993 to 1999 show<strong>in</strong>gseveral features <strong>in</strong>clud<strong>in</strong>g subsidence above a shallow <strong>magma</strong>chamber (M2), <strong>in</strong>flation due to suggested deep <strong>magma</strong> accumulation(M1) <strong>and</strong> a N–S l<strong>in</strong>ear feature relat<strong>in</strong>g to plate spread<strong>in</strong>g.Modified from de Zeeuw-van Dalfsen et al. (2004a).65º10'N65º05'N í1966. The l<strong>in</strong>e was extended to 1.7 km length (Fig. 6)<strong>in</strong> 1968 <strong>and</strong> measured annually until 1972. Annualmeasurements were resumed <strong>in</strong> 1983 <strong>and</strong> the l<strong>in</strong>e wasalso extended. Because not all benchmarks are foundevery year due to snow cover, <strong>and</strong> because the entirel<strong>in</strong>e lies with<strong>in</strong> the deformation field of the volcano,benchmark 404 is arbitrarily set to zero. This po<strong>in</strong>t has<strong>in</strong> recent years been measured annually by GPS.To visualize the changes along this l<strong>in</strong>e we haveplotted the height difference between the end po<strong>in</strong>ts,A429 <strong>and</strong> A406, as a function of time (Fig. 7). StationA406 is 1 km closer to the caldera centre than A429.The data show that the volcano was <strong>in</strong>flat<strong>in</strong>g dur<strong>in</strong>g1970–1972. This had turned to deflation when measurementswere resumed <strong>in</strong> 1983, a trend that hascont<strong>in</strong>ued s<strong>in</strong>ce. The deflation follows an exponential65º00'Nkm0 5 10Öskjuvatn17º 00’W 16º 50’W 16º 40’W5 cmFig. 6. Horizontal GPS-displacements 1993–1998 <strong>in</strong> the Askjavolcano. The model with the two Mogi sources gave an estimateof the displacement of the reference station DYNG (white arrow).The horizontal displacements are adjusted for the displacement ofthe reference station. (Modified from Sturkell et al., submitted forpublication). Inset shows the location of level<strong>in</strong>g benchmarksdescribed <strong>in</strong> the text.

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