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Institut für Mineralogie, University of Münster, Münster, 48149 Germany, putnis@uni-muenster.de
| The first 20% of the full text of this article appears below. |
| INTRODUCTION |
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In the simplest case, we could consider the situation where a mineral, thermodynamically stable under some speciflc temperature and pressure conditions, comes into contact with pure water, such as quartz within its stability field (e.g., at T = 100 °C and 1 atmosphere pressure). Clearly, quartz will tend to dissolve until, at equilibrium, the aqueous silica solution, which at neutral pH is H4SiO4(aq), becomes saturated with respect to quartz. The reaction for this equilibration can be written:
![]() | (1) |
The equilibrium solubility constant for reaction (1) is given by
![]() |
where a(i)aq stands for the activity of the parenthetical aqueous species. For the case of pure quartz and pure water where the activity is 1, Ksp ( qtz ) ~1.2 x 10–3 at 100 °C and 1 atmosphere pressure. However, if under these conditions the solid silica phase in contact with pure water was cristobalite (the high temperature polymorph of SiO2), the resulting aqueous solution, saturated with respect to cristobalite, would be supersaturated with respect to quartz, since the less stable phase is more soluble. The value of Ksp for cristobalite at 100 °C and 1 atmosphere pressure is ~5.1 x 10–3. Thus the thermodynamics would indicate that quartz should precipitate from such a solution. On
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