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124                          Geothermal Energy: Renewable Energy and the Environment


              The decision on what cut-off temperature to use in an assessment will be determined by the
            technology that it is assumed will be available for power generation. As discussed in Chapter 9,
            power generation at temperatures as low as 150°C or less can be accomplished with binary power
            generating systems. However, such systems must also be utilized in settings in which there is suf-
            ficient cooling capacity to meet the thermodynamic aspects of maximizing the delta T between
            production fluid temperature and the cooling capacity of the system. In the assessment performed
            by Williams et al. (2008a), a temperature of 150°C is utilized to define the lower temperature bound
            for defining the reservoir.
              Establishing a reservoir temperature structure is rarely possible, except in instances where wells
            have been drilled and the thermal profile for each well monitored. In the absence of such data, the
            most useful means for estimating the reservoir temperature comes from geothermometers, such as
            those described in Chapter 6. Reed and Mariner (2007) and Williams et al. (2008a) conclude that
            the most reliable geothermometers are the silica, K–Mg, and Na–K–Ca geothermometers. The
            silica geothermometer provides good results, particularly if the formulation of the geothermom-
            eter considers the various effects of different silica polymorphs, as does the method developed
            by Giggenbach (1992). In the temperature range from 90 to 130°C the K–Mg geothermometer
            (Giggenbach 1988) works well, according to the review of results considered by Williams et al.
            (2008a). However, it is often difficult to obtain Mg analyses of sufficient quality and consistency,
            since Mg concentrations can be quite low and are difficult to do at high precision. In the absence
            of Mg analyses, or in waters that are Cl-rich, the Na–K–Ca geothermometer (see Chapter 6 for a
            discussion) is utilized.
              When using such data it is important to keep in mind the limitations of computed temperatures.
            It is generally assumed that the temperature that is obtained from a geothermometer reflects the
            equilibrium chemical composition of the water at the highest temperature the water experienced,
            and that there was, therefore, very little reequilibration of the water as it ascended through the rock
            mass on its way to the surface. The assumptions that equilibrium was achieved and that reequilibra-
            tion did not occur are not wholly justified, since reaction rates do not go to zero once the fluid mass
            passed beyond the thermal maximum. Recall Equation 5.8,


                                  R = S  × k × T  × α × ϕ × ∏a  × (1 − Q/K)            (5.8)
                                                                    ω
                                             fac
                                      A
                                                          i
                                                                                   2
            where R is the rate (moles/s), S  is the effective surface area exposed to the fluid (cm ), k is the
                                      A
            far-from-equilibrium rate constant (moles/cm -s), T is the temperature correction factor for the
                                                 2
                                                      fac
            rate constant k (usually an Arrhenius function), α is a power function that accounts for changes
            in the rate close to equilibrium conditions, ϕ is a function that modifies the rate for precipitation
            relative to that for dissolution that is based on experimental data, a  accounts for the dependence
                                                                   i
            of the rate on the activities of specific components in solution, and ω is power dependence based
            on experimental data that accounts for the particular dissolution or precipitation mechanism.
            Note that in this formulation, R is temperature dependent and thus will not go to zero unless
            equilibrium is achieved at the T of interest. Once equilibrium is achieved, the term k becomes
            zero and R goes to zero, but only for that specific T. As the fluid migrates to lower tempera-
            tures, k is no longer zero, and increases in magnitude as the delta T between the equilibrium
            temperature and the T along the flow path increases. The extent to which reequilibration will
            occur will depend upon the residence time of the fluid in the lower temperature regime and is
            thus dependent on the flow rate—the higher the flow rate, the lower will be the extent to which
            reequilibration takes place.
              These considerations suggest that the computed temperature from a geothermometer is likely to
            underestimate the actual reservoir temperature. The extent to which this is the case is not readily
            determined. For that reason, most geothermometer temperatures used in an assessment should be
            considered conservative.
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