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Exploring for Geothermal Systems                                             99


                               400

                               350

                               300
                              Temperature (°C)  200
                               250



                               150

                               100                   Quartz solubility

                                50

                                 0
                                  0        200      400       600       800
                                                SiO  (aq), mg/kg
                                                   2
            FIGUre 6.7  Comparison of the functional form of the empirical curves for eight different formulations of
            the silica geothermometer used to compute temperatures in Figure 6.6. The solid curve, for reference, is that
            for quartz solubility. (Fournier, R. O., Geothermics, 5:31–40, 1977; Fournier, R. O., Geothermal Systems:
            Principles and Case Histories, New York: Wiley & Sons, Inc., 109–43, 1981; Fournier, R. O. and Potter,
            II. R. W., Geothermal Resources Council Bulletin, 11:3–12, 1982; Verma, S. P. and Santoyo. E., Journal of
            Volcanology and Geothermal Research, 79:9–23, 1997; Arnórsson, S., Isotopic and Chemical Techniques in
            Geothermal Exploration, Development and Use: Sampling Methods, Data Handling, Interpretation, Vienna,
            Austria: International Atomic Energy Agency, 2000; Verma, S. P., Revised Quartz Solubility Temperature
            Dependence Equation Along the Water-Vapor Saturation Curve. In: Proceedings of the 2000 World Geothermal
            Congress, Kyushu, Japan, 1927–32, 2000.)


              controlling SiO  (aq) at temperatures below about 180°C. Whether or not it is, in fact the control-
                        2
            ling phase, or even if a silica polymorph exists in contact with the fluid at the conditions of the
            geothermal reservoir, is unknown until sufficient drilling has been done to elucidate the reservoir
            mineralogy.
              An additional assumption that is problematic, but which must always be invoked, is that the
            ascending waters have not changed their compositional characteristics during ascent to the point of
            sampling. Several processes can occur that will make such an assumption inappropriate. Waters that
            have flashed or have had gases exsolve from them during ascent will invariably have some degree of
            compositional modification through the partitioning of elements between vapor and liquid. Silica,
            in particular, can be significantly impacted by its partitioning into the vapor phase. The extent to
            which this process will occur is not directly evident, however, because exsolution of CO , or its
                                                                                     2
            partitioning into the steam phase will change the fluid pH, which will also indirectly impact silica
            solubility.
              Another  aspect  of  the  assumption  regarding  invariant  composition  during  ascent  is  that  no
            exchange of solutes occurs between the fluid and the surrounding rock within which it is in contact.
            Barton (1984) has shown that for exchange of components in feldspars, reaction times vary between
            hours and years, depending upon the temperature. As previously noted, reaction times are also
            affected by exposed surface area. Fluids that flow sluggishly on their ascent to the point of sampling
            are likely to react to some degree with the host rock. The extent to which that happens remains a
            matter of some debate.
              Finally, the fluid will invariably cool as it comes from depth. Obviously, were that not true, the
            need for geothermometers to estimate the reservoir temperature would be eliminated. Cooling will
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