Jökull


Jökull - 01.12.1957, Side 19

Jökull - 01.12.1957, Side 19
 r/?. j r /r/f. ^ At the end of the activity forming the Mull dike-swarm the local temperature situation at Glasgow may have been as given in Fig. 3. It is assumed that the melting point of basalt Tm is reached at the depth h. Below this depth the temperature gradient is rela- tively small whereas the gradient above the reservoir is relatively large. From the above picture we may subtract the normal tempera- ture field and find an anomalous field as shown in Fig. 4, where Tn is the normal temperature at the depth h. Actually, the adia- batic gradient should be applied below h but this is unimportant. The above model should maximize the tem- perature anomalies. At the end of the volcanic activity we may tentatively assume that the reservoir has largely solidified and that con- duction becomes the main mode of heat trans- fer above as well as below the depth h. The question arises how fast the anomaly given in Fig. 4 decays. The surface heat flow due to the anomaly is easily computed on the basis of equation (30) and is found to be Q1= k(Tm~TAerf(h/2V^) (41) where t is the time since the end of the volcanic activity. By inserting h = 40 km, a = 0.007 cm2/sec and t = 50-106 years we find that the anomaly of the surface heat flow should have decayed to about 60% of the initial value. Thus, if the total present ano- maly at Glasgow amounting to 0.4 microcal/ cm2 sec is due to the above situation its initial value should have been around 0.7. To this figure we may have to add a small contribution from the feeder dikes above the reservoir. In fact, a part of this contribution should be included in the observed anomaly. However, the main influence of the dikes lies at a more shallow depth and, therefore, decays at a faster rate than the anomaly mentioned above. In accordance with the data given above on the relative volume of the dikes the total surface heat flow anomaly due to feeder dikes in Iceland as well as Scotland may at the end of a long period of volcanism amount to as much as 0.3 microcal / cm2 sec provided the dikes extend down to the depth of 40 km. I-Ience, by adding this to the above figure a 17

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