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Jökull - 01.12.1982, Qupperneq 28

Jökull - 01.12.1982, Qupperneq 28
TABLE 1. Estimates ofheat transfer model dimensions for the Reykholtsdalur system. TAFLA 1. Aœtlaðar stærðaríólur um varmajlutning í jarðhitakerjinu í Reykholtsdal. Heat transfer models State Assumed parameters Resulting estimates steady D = 3km, AT = 175°C, d = 1 m Length: 1000 km Single transient t = 3 X 10us, d = 1 m pipe AT = 175°C 700 km steady D = 3 km, e = 0.54, E = 0.70 Area: 2000 km2 Horizontal flow t = 3 X 10us sheet transient e = 0.54 240 km2 t = 3 x 10" Total horizontal Convective downward AT = 200°C fracture length 40 km migration (CDM) in transient C = 5 x 108 J/m3 a vertical fracture M = 3 km Total vertical v = 10-8 m/s contact area 120 km2 A = Effective temperature diíferential General assumptions: Thermal conductivity of formations Thermal diífusivity of formations Local temperature gradient k = 2 W/m,°C a . 10_6m2/s g = 80°C/km really a quite eífective heat transfer element as com- pared to, for example, the horizontal flow sheet. The rather drastic difference between these two models results from the fact that the pipe is supplied by a radial conduction flow, while the sheet is supp- lied by a one-dimensional flow. However, the effec- tiveness of the pipe is greatly reduced in a grid of pipes where oonductive interaction develops. Equa- tion (4) indicates that a sufliciently dense grid of pipes is essentially equivalent to a flow sheet when the spacing satisfies the inequality s«(7rat)1/2/2. Reviewing the results in Table 1, and disregard- ing the single pipe model, we find that the total area estimated for the horizontal flow sheet in a steady state situation is very large. In fact, it would appear diflicult to place this area between the source region and the outlets of the Reykholtsdalur system. More- over, the very serious quesdon arises whether the flood basalt series includes single open flow sheets or interconnected networks of flow sheets of this enormous extent. The transient state flow sheet has a much smaller estimated area and poses therefore fewer problems. Nevertheless, even in this case it is appropriate to question whether the flood basalts series includes open horizontal sheets or networks of sheets ofa few 102km2 area. The CDM model poses the least problems. As a matter of fact, Fig. 1 indicates that 5 dikes outcrop in the area, and we can only surmise that there may be more. Its is quite conceivable that each dike has an effective length of the order of 5 to 10 km where CDM could take place. There would thus appear little difliculty in accounting for the total CDM length of40 km estimated inTable 1. The present discussion can not be extended bey- ond this stage. We can only conclude that the steady state horizontal flow sheet is an unattractive model while its transient counterpart and the CDM model are much more realistic possibilities. On the balance the CDM would appear to have a stronger case. As a matter of course, transient models can be invoked only if there is a plausible cause or explana- tion for the initiation of the processes involved. Referring to the discussion above, this does not appear to be a serious problem as far as LT geo- thermal systems in Iceland are concerned. The 26 JÖKULL 32. ÁR
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