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2.5 Geochemistry  99
                         have little effect on the solubility of quartz and amorphous silica (Fournier and
                         Rowe, 1977). The effects of added salts are significant only for concentrations
                         greater than 2–3 wt% approximately (Marshall, 1980; Fleming and Crerar, 1979;
                                                       ◦
                         Fournier, 1985). However, above 300 C small changes in pressure and salinity
                         become important. The solubility of silica is also affected by pH, for pH values
                         above 7.8–9.3, depending on temperature. However, since pH of geothermal
                         reservoir liquids is generally constrained at values of 5–7 by water–rock reactions,
                         corrections for pH effects are rarely needed in geothermometric calculations. For
                         these reasons, dissolved silica in solutions of near neutral pH from geothermal
                         wells is a reliable geothermometer. The interpretation of dissolved silica from
                         hot springs is somewhat ambiguous because of uncertainties about the mineral
                         controlling dissolved silica and the amount of steam possibly separated (Fournier,
                         1991).
                           Relating the solubility of quartz to enthalpy instead of temperature has several
                         advantages. At a given enthalpy, there is only one value of dissolved silica, while at
                         a given temperature there are two values of dissolved silica, one for the liquid and
                         the other for the steam. The enthalpy can be treated similar to mass, which makes
                         the silica versus enthalpy plot a good tool to investigate isoenthalpic mixing and/or
                         boiling.

                         2.5.7.3 Ionic Solutes Geothermometers
                         A general decrease in Na–K ratios of thermal waters with increasing temperatures
                         was observed long ago (White, 1957; Ellis and Mahon, 1964). The initial attempts
                         to derive, from these observations, an empirical Na–K geothermometer led to
                         equations with relatively small temperature dependences due to the inclusion in
                         the data sets of poorly equilibrated spring waters. It was recognized long ago
                         that Mg contents of thermal waters are strongly dependent on temperature, and
                         this relationship was early attributed to equilibration of geothermal liquids with
                         chlorites (Ellis, 1970) or other Mg-bearing minerals, for example, montmorillonites
                         and saponites.
                           The Na–K–Ca geothermometer (Fournier and Truesdell, 1973) is probably the
                         most popular and used ionic solute geothermometer. The Na–K–Ca function is
                         entirely empirical and assumes two different exchange reactions. The Na–K–Ca
                                                        ◦
                         function gives erratic results below 200 C due to high partial pressures of carbon
                         dioxide (Paces, 1975) and due to the occurrence of exchange reactions involving
                         also Mg. Fournier and Potter (1979) proposed a quite complex Mg correction to the
                         Na–K–Ca function. In addition, precipitation of calcite causes an overestimation
                         of the equilibrium temperature obtained by means of the Na–K–Ca function.
                           However, Reed and Spycher (1984) have suggested that the best estimate of
                         reservoir temperature can be attained by considering simultaneously the state
                         of equilibrium between specific components in water and many hydrothermal
                         minerals as a function of temperature. Therefore, if a group of minerals converges
                         to equilibrium at a particular temperature, this temperature corresponds to the
                         most likely reservoir temperature.
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