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On the pseudobinary join CaO:3MgO:Al2O3:2SiO2:xH2OCaO:1.25MgO:2.75 Al2O3: 0.25SiO2:xH2O clintonite mixed crystals Ca(Mg1+ xAl2 x) (Al4 xSixO10)(OH)2 with x rangingfrom 0.6 to 1.4 occur in the temperature range 600830?C, 2 kb fluid pressure. On the MgSirich side clintonites coexistwith chlorite, forsterite, diopside, and calcite (due to smallamounts of CO2 in the gas phase) and, at lower temperatures,also with idocrase, hydrogrossularite, and aluminous serpentine.Decomposition of clintonite over a divariant temperature rangeoccurs above 830 ?C, 2 kb; clintonite-free subsolidus assemblagescomprising three or four solid phases are formed in the temperatureranges 890 ?1120 ?C. The subsolidus assemblages can berepresented in a polyhedron defined by the corners forsterite,diopside, melilite, spinel, anorthite, corundum, and calciumdialuminate. Above 1120 ?C partial melting occurs. The upper thermal stability limits of three selected compositionshave been reversed in the P-T range 0.520 kb and 7301050 ?C, respectively. Below some 4 kb breakdown is dueto the divariant reactions: (1)Ca(Mg2.25Al0.75)(Al2.75)(Si1.25O10)(OH)2 spinel+diopsidess+forsterite+clintonitess+vapor, (2)Ca(Mg2Al)(Al3SiO10)(OH)2 spinelx002B;melilitess+anorthite+clintonitess+vapor, (3)Ca(Mg1.75Al1.25)(Al3.25)(Si0.75O10)(OH)2 spinel+melilitess+corundum+clintonitess+vapor, At the terminations of the divariant temperature ranges (1)melilitess, (2) diopsidess, and (3) anorthite enter those assemblagesand clintonitess disappears completely. The reactions can berepresented by the following equations (1)log,H2O = 10.28798113/T+0.0856(P1)/T, (2)log = 9.58527325/T+0.0794(P1)/T, (3)log = 7.83585250/T+0.077(P1)/T, with P expressed in bars and Tin ?K. Above 4 kb the upper thermalstability limit of clintonite is defined by incongruent melting,with grossularite participating at pressures above 9 kb. Thesecurves exhibit a very steep, probably even negative slope inthe P-T diagram. There is a close correspondence between natural clintonite-bearingassemblages and thosefound experimentally. The rarity of clintonitein nature is not due to special conditions of pressure and temperaturebut rather due to special bulk compositions of the rocks. 相似文献
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