Jökull


Jökull - 01.12.1964, Side 7

Jökull - 01.12.1964, Side 7
above procedure for computing the thickness of the ice. The largest uncertainty lies in the assumption of a constant regional anomaly, which has to be separated from the effect of the ice-sheet. The use of an infinite sheet- model in calculating the ice-thickness may in- troduce minor errors and will smooth out sub- glacial topographical features which are not large compared with the ice-thickness. Altitudes of some of the stations were determined by an altimeter and may be in error by a few meters. Errors due to this are, however, small in com- parison with the uncertainties mentioned above. A first estimate of the ice-thickness in the Grímsvötn depression and the area east of it may be obtained by assuming a regional ano- maly of —36 mgal here also. This gives a thick- ness of about 110 m near the centre of the depression decreasing to a very srnall value at the ridge at the eastern edge of the depression. The bottom of the depression would then be at an altitude of 1270 meters. Further to the east of Grímsvötn the ice-thickness would, with the same assumption, be 350—400 m with no major variations in the area surveyed. These estimates of absolute ice-thickness in and around the Grímsvötn depression are prob- ably too low, as it is likely from the general picture of the Bouguer anomalies in lceland that the regional anomaly in the Grímsvötn area is smaller than —36 mgal, giving a larger thickness to the ice. It is, however, likely that the variations in ice-thickness in the Grímsvötn area are of the right magnitude. Thus, for in- stance, the height of the subglacial ridge at the eastern edge of the Grímsvötn depression is very likely 150—200 meters above the bottom of the depression. Seismic reflection determinations of ice- thickness have been attempted in the Gríms- vötn depression. Joset and Holtzscherer (1954) give a thickness of 500—700 m at stations in the depression. Unpublished results of J. Martin (Thorarinsson, pers. comm.) indicate a thickness of about 500 m at a station in the eastern part of the depression, and a thickness of about 540 m at a station 3 km southeast of the hut on Grímsfjall. If these thicknesses are correct the regional Bouguer anomaly in the Gríms- vötn area is —10 to —20 mgal instead of the one of —36 mgal, which was deduced near the centre of the profile Grímsfjall towards Kverk- JÖKULL 1964 Fig. 4. fjöll. This would then indicate a somewhat greater ice-thickness near the southwestern end of this profile than is given in Fig. 3. It should be mentioned that the seismic measurements in the Grímsvötn depression are as yet hardly conclusive in regard to ice-thick- ness. Several of these measurements did not yield usable reflections, which is probably due to the very rough topography, which may be expected under the ice in this area. The greatest ice-thickness, 1060 m, which was found by Joset and Holtzscherer on Vatna- jökull, was at a station about 6 km east south- east of Grímsfjall. Such an ice-thickness would contribute about —76 mgal to the total Bouguer anomaly. Although this station is located out- side the area here surveyed, a trend towards larger gravity anomaly would be expected at the gravity stations closest to this seismic sta- tion. Such a trend is not visible on the Bouguer map. CONCLUSIONS Ice-thickness determination by gravity mea- surements depends on the knowledge of the crustal Bouguer anomaly due to the underlying rock formations. This anomaly may be estimat- 65

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