Jökull


Jökull - 01.12.1964, Blaðsíða 6

Jökull - 01.12.1964, Blaðsíða 6
profile Grímsfjall towards Kverkfjöll, and a short profile transverse to it, are shown in Figs. 3 and 4. For computation of the thickness of the ice cap it is necessary to know that part of the Bouguer anomaly, which is due to the mass distribution below sea level. Values as low as —35 mgal were found by Einarsson in the centre of the gravity bowl of Iceland, at the northwestern edge of Vatnajökull. The exact form of the central part of this bowl is not known, as only a limited number of measure- ments is available from the central part of Ice- land. At Jökulheimar the Bouguer anomaly is about —7 mgal according to the present mea- surements. There are thus considerable varia- tions in the regional Bouguer anomalies at the edge of Vatnajökull and they cannot be extra- polated to the Grímsvötn area. Several seismic ice-thickness determinations are available on Vatnajökull from the work of Joset and Holtzscherer (1954). One of their stations (No. 28), which was considered to give reliable results, is located close to the profile line Grímsfjall—Kverkfjöll. Apparently the best procedure available to estimate the ice-thickness along the profile, is to use the known ice- thickness at this station to calculate the re- gional Bouguer anomaly due to the underlying rock formations, and then assume this anomaly to be constant along the profile line. At this station the thickness of the ice was found to be 760 meters, and the Bouguer anomaly —90 mgal. Assuming an infinite ice-sheet of uni- form thickness, the contribution of this sheet to the Bouguer anomaly would be —54 mgal. The remaining —36 mgal would then be due to deeper crustal effects. The ice-thickness on the remaining points of the Grímsvötn—Kverk- fjöll profile and the one transverse to it were then computed from the observed Bouguer ano- malies by subtracting an assumed regional ano- maly of —36 mgal and using a conversion factor of 14.0 m/mgal, which is valid for an infinite sheet of density difference 1.7 g/cm3. Several sources of error are possible in the JÖKULL 1964 64

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Jökull

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