Jökull


Jökull - 01.01.2016, Side 37

Jökull - 01.01.2016, Side 37
First documented surge of Kverkjökull, central Iceland Figure 5. Slope maps (A) for 2007 and 2011 both depicting increased crevassing and serac formation in 2011 compared to 2007. The leading edge of the most chaotic ice surface in 2011 is outlined with a white dashed line in A and forms a coherent lobe shape. The combination of changing slope and changing ice thickness produced a change in driving stress (B). In B, note the spatial pattern and zones of low (L), medium (M) and high (H) relative changes in driving stress as annotated and delimited by dashed white lines. – Hallakort (A) sýna um- fangsmeiri sprungusvæði og ísturna árið 2011 en 2007. Jaðar uppbrotna svæðisins árið 2011 er afmarkaður með hvítri, slitinni línu í A sem sýnir að framhlaupið myndar tungu niður miðjan jökulinn. Breytingar í halla og ísþykkt leiða hlutfallslega til lítillar (L), nokkurrar (M) og mikillar (H) breytingar í botnspennu á svæðum sem afmörkuð eru með hvítum, slitnum línum (B). to the alignment of ridges in the ice-free topography. It is possible that the surge only affected the south- westerly part of the terminus region for some dynam- ical reason and that the increased crevassing and am- plified hummocky ice-surface undulations are formed at the boundary between ice affected and unaffected by the surge. There are many examples in Iceland of surges affecting only a part of the corresponding ice- flow basin as further discussed below. Therefore, we contend that the asymmetric pat- tern of surface elevation changes in the terminus area of Kverkjökull between 2007 and 2011 is best explained by a hypothesis of a different speed of surge front propagation between the north-eastern and south-western portions of the terminus. The surface expression of this more rapid front propagation in the south-western part of the terminus area is more widespread and more intensely hummocky surface texture of the 2011 DEM, as depicted in slope maps (Figure 5A) and elevation range maps (Figure 6), and field photographs (Figure 7), as well as increased depth of crevasses and height of seracs. Quantita- tively, crevasses and seracs had local relief in adjacent grid cells (i.e. over 10 m horizontal distance) of <8 m in 2007 but up to 18 m in 2011, and local relief of >5 m is found over 80% of the example transects in 2011 compared with <10% in 2007 (Figure 6). In the field, those accessible had the form of stacked thrust blocks revealed by exposed thrust planes between rel- atively ‘clean’ and ‘dirty’ ice (Figure 7). The com- bination of changing slope gradient (Figure 5A) and changing ice thickness produced a change in the driv- ing stress with a relatively complicated pattern, which can be interpreted to have zones of relatively high and low changes in driving stress (Figure 5B). Notably, a ‘corridor’ of relatively little change in driving stress, JÖKULL No. 66, 2016 37
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Jökull

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