Page 142 - Geothermal Energy Renewable Energy and The Environment
P. 142

128                          Geothermal Energy: Renewable Energy and the Environment


                               1.0

                               0.8
                              Fraction of total flow  0.6  Dixie valley B-T model



                               0.4


                               0.2           Beowawe


                               0.0
                                 0.0     0.2     0.4    0.6     0.8     1.0
                                           Fraction of permeable volume
            FIGUre 7.5  The curves in this figure compare the proportion of flow for which a given fraction of the per-
            meable volume of a reservoir is responsible. The curves for Beowawe (Shook 2005) and Dixie Valley (Reed
            2007) are based on the fractal model discussed by Williams (2007) and Williams et al. (2008a). The curve
            labeled “B-T model” is the relationship based on the Bodvarsson and Tsang (1982). (Modified from Williams
            et al. 2008a; Bodvarsson, G. S. and Tsang, C. F., Journal of Geophysical Research, 87, 1031–48, 1982.)


            is unlikely. Hence, pressure differences will develop throughout the flow field that will affect the
            flow  pattern,  diminishing  the  efficiency  with  which  heat  can  be  extracted  uniformly  from  the
            reservoir.
              Finally, the treatment represented in the figure does not capture the behavior of a fractured
            medium. If fluid production is primarily through fracture flow, then the main pressure drop in the
            reservoir will be within the fractures. Perpendicular to the fracture surfaces there will be an addi-
            tional pressure differential in the porous medium that is the rock, and fluid movement from the rock
            to the fracture may occur, albeit at a rate significantly lower than in the fracture. This movement of
            fluid from porous medium to fracture is likely to be small, but will not necessarily be zero. Hence,
            a certain amount of convective heat transfer will occur between rock and fracture, in addition to
            that expected from simple conduction. Nevertheless, the spacing and abundance of fractures will
            dominate the ability of heat to be extracted from the reservoir. The greater the interface area that is
            exposed along fractures in the reservoir, the greater will be the recovery factor. However, as noted
            in the references above, the effectiveness of this extraction process generally results in a recovery
            factor that is modest for fractured reservoirs.
              The most successful means for mathematically representing the relationship between fracture
            flow on the recovery factor was developed by Williams (2007) who used a fractal approach for
            describing the interaction. Consideration was given to the proportion of flow in various fracture
            populations in a system. The results of the model were consistent with the observed behavior for
            well-characterized, fracture-dominated systems. Figure 7.5 represents the results using this approach
            for Dixie Valley and Beowawe, both of which are fracture-dominated geothermal reservoir systems.
            The curves document that a small proportion of the fractures carry a disproportionately high vol-
            ume of the flow—at Dixie Valley 35% of the flow is accommodated by 10% of the fracture perme-
            ability, while at Beowawe that value is 50% of the flow in 10% of the fracture permeability. Since
            such a small proportion of the total fractures account for a large proportion of the flow, there will
            be a significant volume of the geothermal reservoir in which interaction with the fracture regime
            will be minimal. As a result, extraction of heat will not be uniform and the recovery factor will be
            relatively low.
   137   138   139   140   141   142   143   144   145   146   147