THE SOLUBILITY OF ELEMENTAL MERCURY IN WATER
The solubility of elemental mercury (Hg') at temperatures between 30 and 210°C was determined by direct sampling of mercury saturated water contained in a fixed volume stainless steel autoclave. The temperature dependence of the solubility was best represented by the equation log,^^, = -11.879 + 0.01206T where xHg is the mole fraction of dissolved Hgo and T is the temperature in degrees Kelvin. At temperatures less than 100°C the best literature values are in good agreement with these results. At higher temperatures it is difficult to compare our data with previous studies as they show widely divergent results. Comparison of field results for volatile mercury steam/water partitioning showed that up to 10' times more mercury was retained in solution than would have been indicated from the theoretical distribution coefficients calculated from the solubility data. A kinetic limitation to the mercury steadwater distribution in the Webre separator was the most likely explanation although the presence of other nonvolatile mercury species could not be discounted. INTRODUCTION The ability to predict the transport and partitioning behaviour of elemental mercury (Hg') during exploitation of geothermal reservoirs and power production requires reliable data for the vapour/liquid distribution coefficients. The distribution coefficient is derived from Henry's law constant which can be calculated from the solubility of elemental mercury. This study was undertaken because the large differences in Hgo solubility values between the few published experimental studies at temperatures above 100°C made it difficult to interpret field data collected at the Ohaaki geothermal field (Timperley and Mroczek 1989). The importance of elemental mercury is that it appears to be the dominant chemical form of mercury found in chemical surveys of wells at New Zealand geothermal fields. This is in agreement with previous studies (Robertson et al. 1978) which showed that most if not all the mercury present in geothermal effluent is Hg', even at high H,S gas levels. Chemical modelling (Varekamp and Buseck 1984) has also shown that mercury transport occurs largely as Hgo in dilute hydrothermal systems 'with moderate amounts of S (<0.01 mol/litre). PREVIOUS WORK At temperatures less than 100°C there have been numerous experimental solubility studies using a variety of measurement techniques. These studies also show a wide variation in values. The reason for the disagreement is not clear but trace contamination by air oxygen or not enough time allowed to attain the equilibrium solubility are commonly suggested reasons. Clever et al. (1985) reviewed and evaluated all available data and presented smoothed solubility data and smoothed Henry's constant equations over the temperature interval 273.15-393.15 K. The only high temperature study included in their evaluation was that of Sorokin (1973). Sorokin measured the solubility of mercury in water at temperatures of 573, 673 and 773 K at total pressures between 507 and 1013 bar. Samples were extracted from a flexible reaction cell autoclave at constant pressure and temperature. Clever et al. (1985) combined the hypothetical Henry's constant at the higher temperatures extrapolated to 1 bar with the Henry's constants calculated from the lower temperature data (277-346 K) of Clew and Hames (1971) to obtain an equation for Henry's constant over the temperature interval 393-773 K. Varekamp and Buseck (1984) also used the thermodynamic parameters calculated from Clew and Hames's (1971) data as well as Sorokin's (1973) data to calculate the solubility of Hgo to 250°C. Recently Gushchina et al. (1989) determined the solubility of mercury using a spectrophotometric technique at temperatures of 150,200 and 250°C as well as evaluating previous work. Their results as well as those of Sorokin (1973), Sorokin's more recent experimental results and calculations as reported by Gushchina et al., Varekamp and Buseck's (1984) extrapolations, the smoothed literature interpolations of Clever et al. (1985) as well as selected low temperature
HEAT CAPACITY OF LIQUID MERCURY BETWEEN 0 AND 450 C CALCULATION OF CERTAIN THERMODYNAMIC PROPERTIES OF THE SATURATED LIQUID AND VAPOR
The enthalpy of liquid mercury was measured from 0° to 450° C by the "drop" method . These and other precise published data were used to calculate a number of the rmodynamic properties of liquid and gaseous mercury at the vapor pressures from the triple point , 38.88°, to + 500° C. The entropy calculated from data on the vapor and liq uid was compared with that derived from published low-temperature heat-capacity data for the solid . The calculated values of vapor pressure, also using data on the vapor and liquid, were fo und to agree over a wide temperature range with certain published experimental values when independently derived gas-imperfection and published temperature-scal e corrections were applied.
Time and Heritage
As a historian studying what can be considered a form of intellectual history, I have slowly come to adopt Michel de Certeau’s observation made at the end of the 1980s that ‘objectifying the past, for the last three centuries, has undoubtedly left unconsidered time within a discipline that has continued to use it as a taxonomic instrument’. To a certain degree, time has become commonplace for the historian who has preserved or instrumentalized it. It is not considered because it is inconceivable, but because we do not think of it or, more simply, we do not think about it. As a historian attempting to pay attention to the time I’m living in, I have thus, like many others, noticed the swift development of the category of the present until it has become obvious that the present is omnipresent. This is what I refer to here as ‘presentism’.