Jökull


Jökull - 01.12.1961, Page 39

Jökull - 01.12.1961, Page 39
discussion of similar topics in the case of the Wairakei thermal area in New Zealand, the reader is referred to the fine papper of Studt (1958). For the sake of completeness, a point of major interest will be discussed briefly. The drilling carried out in the thermal areas of Iceland has revealed the important fact that the heat output of the wells can surpass the natural output of the area before drilling. An increase by a factor as high as 20 has been ob- tained in one case. This poses the important problem as to the origin of the additional flow of heat ancl water. It is possible that the wells may induce a considerable decrease of the natural impedance of the flow and thus lead to an increased circul- ation in the entire hydrothermal system. On the other hand, a transitory increase of the flow can also be obtained on the basis of the large amount of heat accumulated in the up- flow zones of the individual areas. The density of water decreases with increasing temperature, mainly above 100° C. The density of water at 100° C is 0.96 gr/ml, at 200° C 0.87 and at 250° C only 0.80. Therefore, cold water in the formations surrounding the thermal areas has a tendency of encroaching on the hot water within the discharge zone to drive it out. How- ever, the cold water entering the hot rock is heated by the contact with the rock and new hot water is formed. This transitory circulation can, therefore, be maintained by the surplus heat in the rock and will last as long as there is surplus heat present.. Moreover, the steam flow from wells in high- temperature areas may partially depend on the boiling of pore-water in the hot rock. Porous rock at temperatures above 100° C and satura- ted with water can act as a lieat reservoir in a somewhat different way. Wells drilled into the rock may induce a decrease of pressure ancl a subsequent boiling of the water in the pores. At a not too great porosity the boiling will largely depend on the heat content of the rock. As a matter of course, the temperature of the rock has to be near to the boiling tem- perature of water at the depth of the rock formations. Both types of heat reservoirs may be encountered in the high-temberature areas. The present author (Bodvarsson, 1956) has estimated the total potentialities of thermal areas in Iceland lor power production at sóme 300 megawatts steady power and a reco- verable lieat reservoir of some 15,000 mega- wattyears. At present natural heat is utilized in Ice- lancl mainly for domestic and green-house heating. The total amount of heat utilized corre- sponds to a yearly saving of fuel oil of approxi- mately 60.000 metric tons, that is, about 350 kilograms per vear per capita. 6. GEOPHYSICAL EXPLORATION OF THE NATURAL HEAT RESOURCES. Geophysical exploration has been of con- siderable importance for the development of the natural heat resources of Iceland. In some cases the exploration work has been of a deci- sive importance. A review of the methods in- volved and a number of case histories have been given elsewhere by the present writer (Bodvarsson, 1950). For detailed information the reader is referred to this paper. The geophysical exploration is carried out mainly for two purposes. Firstly, for the un- covering of structural features. Secondly, for the study of the subsurface temperature field. The latter methods are generally referred to as the direct methods, whereas the structural methods represent the indirect methods. The indirect methods involve the convent- ional technique as the magnetic, gravitational and the seismic methods. Their application to the natural heat prospecting does generally not differ much from the methods of prospecting for oil and minerals. The main purpose is the uncovering of intrusives, mainly dikes, and tec- tonic structures. The introduction of the seismic methods for the study of the flood basalts represents probab- ly the main advance during the past 10 years. For further information the reader is referred to the papers by Báth (1960) and by Báth and Tryggvason (1961). The direct methods involve a technique spe- cially adapted to the natural heat prospecting. The main purpose is the study of the subsurface temperature field, mainly the base temperature and the extension of the rock heated to this temperature. The methods involve the thermal, the electric resistivity and the geochemical met- 37

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