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Dept. Erdwissenschaften, ETH Zürich, Institute for Mineralogy & Petrology,Clausiusstrasse 25, Zürich, CH-8092, Switzerland
| The first 20% of the full text of this article appears below. |
| INTRODUCTION TO NATURAL IMMISCIBLE SYSTEMS |
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Although the main emphasis in this volume is on fluid–fluid equilibria, there are good examples and much literature on liquid–liquid equilibria in synthetic silicate melts and natural magmas. In fact much of our understanding of phase separation (for geochemists generally taken simply as liquid–vapor equilibria) actually originates from liquid–liquid immiscibility studies of silicate melts. For a one-component system there are three distinct regions in PT space where either solid or liquid or vapor exist as the stable phase. These are separated by three univariant curves (i) the solid–liquid curve, the solidus, (ii) the liquid–vapor curve, which can lead to the most commonest form of critical point (see Fig. 1a
), and (iii) the solid–vapor curve, which reflects direct vaporization (sublimation) or condensation of solids from gas. The latter is relevant in some industrial processes and to condensation of stars at vacuum pressures. For each added component with solid, liquid and vapor phases, there is the possibility of mixing of each of the phases, or not. In silicates we are used to recognize immiscibility gaps (solvus) among chemically related minerals (e.g., alkali feldspars), which are miscible at high temperatures in the subsolidus region but are immiscible with cooling and undergo phase separation. We are less used to consider immiscibility between two anhydrous melts (silicate–silicate, silicate–carbonate, silicate–oxide, silicate–sulfide,
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