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1 Department of Earth and Planetary Sciences, Johns Hopkins University, Baltimore, Maryland 21218, U.S.A.
2 Department of Earth and Space Sciences, University of California at Los Angeles, Los Angeles, California 90095, U.S.A.
Correspondence: * E-mail: jferry@jhu.edu
| The first 20% of the full text of this article appears below. |
The P-T conditions of both equilibria were determined precisely by reversal experiments in a piston-cylinder apparatus. On the basis of 8 experiments, brackets for the rutile-magnesite-geikielite equilibrium are 7.07.1 kbar at 800 ° C, 8.68.7 kbar at 850 ° C, and 10.510.7 kbar at 900 ° C. On the basis of 9 experiments, brackets for the zircon-magnesite-baddeleyite-forsterite equilibrium are 7.17.7 kbar at 800 ° C, 9.29.4 kbar at 850 ° C, and 10.710.9 kbar at 900 ° C. Considering experimental uncertainties in P (±300 bars) and T (±3 ° C), equilibrium curves calculated from both the Berman and the Holland and Powell databases pass through all brackets. Molar Gibbs free energy of formation from the elements at 1 bar and 298 K for geikielite and zircon, derived from the experiments and consistent with the Berman database, are 1481.94 ± 0.67 kJ and 1917.54 ± 1.25 kJ, respectively. Corresponding values consistent with the Holland and Powell database are 1479.30 ± 0.74 kJ and 1918.47 ± 1.49 kJ. Application of the two equilibria indicate that: (1) the mole fraction of CO2 in fluid was 0.541.00 when geikielite and baddeleyite formed during contact metamorphism of siliceous dolomites in the Ballachulish aureole, Scotland; (2) the activity of CO2 could have been as low as 2·105 during ultra-high pressure metamorphism of magnesite-bearing ecologites; and (3) the activity of CO2 was <0.18 during one instance of mantle metasomatism.
| INTRODUCTION |
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![]() | (1) |
and
![]() | (2) |
[these and all other abbreviations for minerals follow Kretz (1983)]. Isograds can be mapped in contact aureoles based on reactions 1 and 2, and they lie at grades above that of
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