Jökull


Jökull - 01.12.1957, Side 32

Jökull - 01.12.1957, Side 32
Fig. 6. Dirt band outcropping on the forward slope of a ridge on Svínafellsjökull, below the icefall. On the crest of the ridge can be seen one of the ice arches. Aurborfíi á Svinafellsjökli. new winter snow and ice could be turned through an angle to outcrop at the surface along only a comparatively thin line. A further suggestion has been made that the inclined dirt layers may be due to dirt which has lodged in crevasses on the icefall in the summer. This might be expected to produce a great number of dirt bands of no great length of density, but on Svínafellsjökull we found that the dirt bands were spaced well apart with no sign of dirt lines in between, and we found them quite high up the foot of the icefall, where, if they had originated in the bottoms of crevasses, the ablation had not been great enough to expose the dirt. Yet it must be admitted that dirt lodges in crevasses on the icefall would produce many of the necessary features of multiple ogives — the faint but wide dirt distribution, the seasonal rhythm due to chang- es of ablation on the fast moving iceíall and the striped nature of the ogive. The second solution which suggested itself was that ogives are in fact thrust planes, to which they are outwardly so similar. Chamber- lin (10), Lewis (11) and Miller (12) have all noted the three-dimensional nafure of ogives, and related them to possible zones of thrusting. In their study of Morsárjökull’s single ogives Ives and King noted that “the presence of the discrete surface at the top of the dirty band and in some cases also at its base may suggest that overthrusting or rotational slipping is an important process in the formation of the ogives”. At periods of maximum ice supply down the icefall the inertia of the glacier at the bottom may be such that pressure builds up in the icefall, and is released by shearing and overthrusting of ice, along zones of max- imum shear stress. A number of difficulties arise in connection with this theorv, although it can be shown to satisfy most of the require- ments. The first difficulty is that of differentiating between a thrust plane in which dirt has been brought up from the glacier bed, and a thrust plane that has developed along a dirty layer already present in the ice. This difficulty is equally evident when studying apparent thrust planes at glacier snouts. Granted that stresses in the ice may occasionally rise to a point where shearing could take place (which is doubtful), such shearing woulcl occur at the weakest point. It might be along the theoreti- cal line of maximum shear stress, or it might take advantage of a tectonic band or dirt layer already present and constituting a line of weak- ness.The latter may be the case on Morsárjökull’s avalanche fan, where the regenerated stratifica- tion layers provide excellent surface of weak- ness. Thus in one case a dirt layer may be the cause of shearing occurring at that point, in another it may be the result. According to Nye’s classification (7) the cre- vasse pattern below the icefalls of the three glaciers studied is longitudinal, suggesting a zone of compressive flow. This may be as- sociated with curved surface of maximum shear stress within the ice along which thrusting could develop, carrying up dirt from the bed of the glacier. The next question is to decide what order of magnitude the thrusting must be to originate ogives that outcrop at the sur- face. If one assumes that the main activity occurs below the foot of the icefall a very large vertical movement is necessary. However, the highest evidence of a single ogive found on Svínafellsjökull was high up the lower part of the icefall, and the single ogive bands were already well developed at its foot. This sug- gests that thrusting might occur in the icefall itself, at the change of slope below the main avalanche zone. The diagram (fig. 7) shows the sort of pro- 30

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