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1.
The System CaO-CO2-H2O and the Origin of Carbonatites   总被引：2，自引：0，他引：2  
The ternary isobaric (TX) prism for the system CaO–CO2–H2Owas determined at 1,000 bars pressure between 600? C and 1,320?C. At this pressure, calcite melts incongruently at 1,310? C,portlandite (Ca(OH)2) melts congruently at 835? C, a binaryeutectic exists between calcite and portlandite at 685? C, meltingbegins at 740? C on the join calcite-water and the univariant(isobaric invariant) equilibria lime?calcite?portlandite?liquidand calcite?portlandite?liquid?vapour occur at 683? C and 675?C, respectively. The latter is the minimum liquidus temperaturein the TX prism, and the composition of this liquid is 65CaO,19CO2, 16H2O (in weight per cent). PT curves were determinedfor several univariant equilibria. In the binary system CaO-H2O,four univariant curves meet at an invariant point, at 810? Cand 100 bars pressure. Portlandite dissociates only at pressuresbelow this point. The minimum liquidus temperature in the ternarysystem varies between 685? C and 640? C in the pressure interval27 bars to 4, 000 bars. Liquids in the system are regarded as simplified carbonatitemagmas in which CaO represents the basic oxides, and CO2 andH2O the volatile constituents. The liquids have low viscosityas indicated by the rapid attainment of equilibrium and theobservation that crystal settling takes place in 15-min runs.The existence of such liquids at moderate temperatures througha wide pressure range leaves little reason to doubt a magmaticorigin for those carbonatites which appear to be intrusive.Differentiation could occur in multicomponent magmas by separationof the successive liquid fractions produced by crystallizationof calcite, dolomite, and siderite. The determined phase relationsdo not favour an origin by gas transfer. The results also suggestthat partial melting of limestones is likely at igneous contacts,and that impure limestones may be partially melted during high-graderegional metamorphism.  相似文献   

2.
Phase relationships on the vapor-saturated liquidus surfacein the system CaO-MgO-CO2-H2O have been deduced from data inthe systems CaO CO2-H2O, CaO-MgO-CO2, and MgO-CO2-H2O, and frompreliminary experiments in the quaternary system. These areillustrated in composition tetrahedra, and in isobaric sectionsthrough the petrogenetic model. The univariant PT curve forthe beginning of melting lies between 625? C and 600? C in thepressure range 10 bars to 4 kilobars, in the presence of a vaporphase rich in H2O. The curve is divided into three sectionsby two invariant points, each section having a different primarymagnesian phase involved in the melting reaction. Periclaseoccurs on the low-pressure section (less than about 1 kilobar),and with increasing pressure first brucite and then dolomitebecome stable on the liquidus. The pressure of the second invariantpoint, above which dolomite is stable on the liquidus, is notknown. The effect of FeO as an additional component is considered.Processes of crystallization resulting from changes in temperature,in pressure, and in the composition of the vapor phase are discussed.These processes are applied to the crystallization and differentiationof carbonatite magmas, and the reverse processes involving fusionare applied to the metamorphism of dolomites. Crystallizationdifferentiation of a carbonatite magma could produce the sequenceof intrusion observed at some carbonatite complexes: calcitics?vite, followed by ankeritic s?vite, and finally sideriticcarbonatite. Partial melting may occur during the thermal metamorphismof dolomites, but melting is unlikely during regional metamorphism.  相似文献   

3.
The solubility of water in a basaltic and in an andesitic melthas been determined in the pressure range from approximately1,000 to 6,000 bars at 1,100? C. The solubility in basalticmelt is 3.1 weight percent at 1,000 bars and 9.4 weight percentat 6,000 bars; in the andesitic melt it is 4.5 weight percentat 1,000 bars and 10.1 weight percent at 5,300 bars. The temperaturesof appearance of the primary, secondary, and tertiary phasesin the basalt have been determined at 1,000 bars water pressureand at the fo2's of the magnetite+hematite (MH), magnetite+fayalite+quartz(MFQ) and magnetite+w?stite (MW) buffers. Results are as follows: Buffer Pyroxene Plagioclase Ore mineral MH 1,095?C 1,065?C 1,230?C MFQ 1,040? 1,015? 1,010? MW 1,020? 1,010? 995? A comparison of the solubility of water at 1,100?C and up toapproximately 6,000 bars pressure in several silicate melts,ranging in composition from granitic to gabbroic, indicatesthat the spread of solubility is narrower than has been supposed.The marked effect of fo2's on the crystallization sequence inthe Columbia River basalt confirms the importance of this factorin determining liquid lines of descent. In experiments withlow fo2's (MW buffer) and 1,000 bars water pressure, the basaltwas completely liquid at the relatively low temperature of 1,020?C.  相似文献   

4.
The Synthesis and Stability of Anthophyllite   总被引：1，自引：1，他引：0  
The pure magnesium orthorhombic amphibole, anthophyllite, hasbeen synthesized and its upper and lower stability limits havebeen established by reversible hydrothermal experiments. Thesynthetic mineral has refractive indices nx=1?587?0?001, ny=1?602?0?005,nz=1?613?0?001, and unit-cell dimensions of a0=18?61?0?02 ?,b0=18?01?0?06 ?, c0=5?24?0?01 ?. The mineral is stable overa narrow temperature range in the presence of the phase H2O.At a PH2O of 1,000 bars the upper stability limit is 745??10?C and the lower stability limit is 667??8? C. Rate studies indicate that anthophyllite can nucleate at temperaturesabove its upper stability limit by disintegration of talc sheetsinto strips of double chains. The activation energy for thisprocess is 150?30 kcal mol–1. Application of the data to rocks of the Balmat area, New York,suggests that the equilibrium pressure of water during the metamorphismwas significantly less than the total pressure. The data indicatethat monomineralic zones of anthophyllite in ultramafic rocksare due to the presence of a steep gradient in the activityof H2O, or a steep gradient in temperature, or both, acrossthe zones.  相似文献   

5.
On the pseudobinary join CaO:3MgO:Al2O3:2SiO2:xH2O–CaO: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 600–830?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 0.5–20 kb and 730–1050 ?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 = 10.2879–8113/T+0.0856(P–1)/T, (2)log = 9.5852–7325/T+0.0794(P–1)/T, (3)log = 7.8358–5250/T+0.077(P–1)/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   

6.
Equilibrium H2O pressure (PeH2O) was fixed at values less thantotal pressure (PT) in melting experiments on mixtures of 1921Kilauea tholeiite, H2O, and CO2 (58.5 mole per cent H2O, 41.5mole per cent CO2), buffered by Ni+NiO. New determinations ofthe beginning of melting of mixtures of 1921 Kilauea tholeiiteand H2O buffered by quartz+fayalite+magnetite were made at 2and 3 kb. Microprobe analyses of coexisting glass, clinopyroxene,?olivine, ?amphibole were determined for several runs. Decreasing H2O fugacity (fH2O) to about six-tenths the fugacityof pure H2O (f?II2O) raises the solidus and the upper stabilitylimit of plagioclase. Plagioclase and clinopyroxene coexistin equilibrium with liquid-a feature not observed in the pureH2O system. Amphibole is stable to about 970 ?C at 2 kb, 1025?C at 5 kb and 1060 ?C at 8 kb. The Al (VI)+Ti contents of theamphibole increase with P, yielding kaersutite at 1050 ?C and8 kb. Calculated modes for the condensed phases reveal large differencesin the amount of glass (liquid) present and large differencesin liquid composition below and above the breakdown temperatureof amphibole at 5 and 8 kb. Liquids coexisting with amphibole,clinopyroxene, olivine, and magnetite are dacitic near the solidusand silica-rich andesites around 1000 ?C at 5 and 8 kb. Theresults of this study substantiate the model for the generationof the calc-alkaline suite by partial melting of H2O-rich basalts.  相似文献   

7.
Hydrothermal experiments on natural samples of trachyandesiteand dacite bulk composition show that anhydrite (CaSO4) mayoccur as a stable phenocryst phase at oxygen fugacities greaterthan or equal to 1.0 to 1.5 log fO2 units above the Ni–NiOequilibrium. The dissolved sulfur concentration in anhydritesaturated melts from MnO–Mn3O4 buffered experiments decreaseswith decreasing temperature, from approximately 2300 p.p.m.Sat 1025?C to 250 p.p.m.S at 850?C (all at 2 kb Pfluid = Ptotal).In FeS-saturated melts equilibrated at the Ni–NiO bufferand 2 kb pressure, the concentration of dissolved sulfur alsodecreases with decreasing temperature, varying from approximately400 p.p.m. S at 1025?C to less than 100 p.p.m. S at 850?C. AtNNO or lowerfO2s, decreasing melt FeO content due to crystalfractionation may explain the observed decrease in sulfur solubilitywith decreasing temperature. Sulfur solubility values equivalent to the approximately 0.6wt. per cent S present in fresh bulk pumice samples from the1982 eruptions of El Chichon volcano are not readily achievedunder any reasonable combinations of pressure, temperature,and oxidation state. Dissolved sulfur contents approaching 0.6wt. per cent might occur if the source regions of melts parentalto the El Chichon trachyandesite were at an fO2 several logunits above the Ni–NiO equilibrium. Because such elevatedoxidation states are far greater than the generally acceptedvalues for mantle-derived partial melts we believe the highsulfur content of the El Chichon pumices is not a primary feature;it reflects reaction with sulfur enriched material at some unknowndepth beneath the volcano. Published sulfur isotopic and petrologicdata suggest that hydrothermally altered rocks similar to thepyrite- and anydritebearing lithic fragments found in the 1982pumices could have provided a source of sulfur for crystallizationof magmatic anhydrite. The anhydrite was an important sourceof sulfur for evolution of a sulfur-rich vapor phase duringeruption of the magma. Although many calc-alkaline dacites and rhyolites appear toattain oxidation states high enough to stabilize anhydrite,the characteristically low bulk sulfur contents of these rockswill limit anhydrite abundances to less than approximately 0.1wt. per cent, assuming sufficient sulfur is present to achievesaturation. Such small amounts of a water soluble mineral couldbe easily removed by subaerial weathering processes, dissolvedduring vapor exsolution from a magma, or simply overlooked duringroutine petrographic examination.  相似文献   

8.
Four natural peridotite nodules ranging from chemically depletedto Fe-rich, alkaline and calcic (SiO2 = 43.7–45.7 wt.per cent, A12O3 = 1.6O–8.21 wt. per cent, CaO = 0.70–8.12wt. per cent, alk = 0.10–0.90 wt. per cent and Mg/(Mg+Fe2+)= 0.94–0.85) have been investigated in the hypersolidusregion from 800? to 1250?C with variable activities of H2O,CO2, and H2. The vapor-saturated peridotite solidi are 50–200?Cbelow those previously published. The temperature of the beginningof melting of peridotite decreases markedly with decreasingMg/(Mg+SFe) of the starting material at constant CaO/Al2O3.Conversely, lowering CaO/Al2O3 reduces the temperature at constantMg/(Mg+Fe) of the starting material. Temperature differencesbetween the solidi up to 200?C are observed. All solidi displaya temperature minimum reflecting the appearance of garnet. Thisminimum shifts to lower pressure with decreasing Mg/(Mg + Fe)of the starting material. The temperature of the beginning ofmelting decreases isobarically as approximately a linear functionof the mol fraction of H2O in the vapor (XH2Ov). The data alsoshow that some CO2 may dissolve in silicate melts formed bypartial melting of peridotite. Amphibole (pargasitic hornblende) is a hypersolidus mineralin all compositions, although its P/T stability field dependson bulk rock chemistry. The upper pressure stability of amphiboleis marked by the appearance of garnet. The vapor-saturated (H2O) liquidus curve for one peridotiteis between 1250? and 1300?C between 10 and 30 kb. Olivine, spinel,and orthopyroxene are either liquidus phases or co-exist immediatelybelow the temperature of the peridotite liquidus. The data suggest considerable mineralogical heterogeneity inthe oceanic upper mantle because the oceanic geotherm passesthrough the P/T band covering the appearance of garnet in variousperidotites. The variable depth to the low-velocity zone is explained byvariable aHjo conditions in the upper mantle and possibly alsoby variations in the composition of the peridotite itself. Itis suggested that komatiite in Precambrian terrane could formby direct melting of hydrous peridotite. Such melting requiresabout 1250?C compared with 1600?C which is required for drymelting. The genesis of kimberlite can be related to partial meltingof peridotite under conditions of XH2Ov = 0.5–0.25 (XCO2v= 0.5–0.75). Such activities of H2O result in meltingat depths ranging between 125 and 175 km in the mantle. Thisrange is within the minimum depth generally accepted for theformation of kimberlite.  相似文献   

9.
Four natural peridotite nodules ranging from chemically depletedto Fe-rich, alkaline and calcic (SiO2=43?7–45?7 wt. percent, Al2O3=1?6O–8?21 wt. per cent, CaO=0?70–8?12wt. per cent,alk=0?10–0?90 wt. per cent and Mg/(Mg+Fe2+)=0?94–0?85)have been investigated in the hypersolidus region from 800?to 1250?C with variable activities of H2O, CO2, and H2. Thevapor-saturated peridotite solidi are 50–200?C below thosepreviously published. The temperature of the beginning of meltingof peridotite decreases markedly with decreasing Mg/(Mg+Fe)of the starting material at constant CaO/Al2O3. Conversely,lowering CaO/Al2O3 reduces the temperature at constant Mg/(Mg+Fe)of the starting material. Temperature differences between thesolidi up to 200?C are observed. All solidi display a temperatureminimum reflecting the appearance of garnet. This minimum shiftsto lower pressure with decreasing Mg/(Mg+Fe) of the startingmaterial. The temperature of the beginning of melting decreasesisobarically as approximately a linear function of the mol fractionof H2O in the vapor (XH2O). The data also show that some CO2may dissolve in silicate melts formed by partial melting ofperidotite. Amphibole (pargasitic hornblende) is a hypersolidus mineralin all compositions, although its P/T stability field dependson bulk rock chemistry. The upper pressure stability of amphiboleis marked by the appearance of garnet. The vapor-saturated (H2O) liquidus curve for one peridotiteis between 1250? and 1300?C between 10 and 30 kb. Olivine, spinel,and orthopyroxene are either liquidus phases or coexist immediatelybelow the temperature of the peridotite liquidus. The data suggest considerable mineralogical heterogeneity inthe oceanic upper mantle because the oceanic geotherm passesthrough the P/T band covering the appearance of garnet in variousperidotites. The variable depth to the low-velocity zone is explained byvariable aH2O conditions in the upper mantle and possibly alsoby variations in the composition of the peridotite itself. It is suggested that komatiite in Precambrian terrane couldform by direct melting of hydrous peridotite. Such melting requiresabout 1250?C compared with 1600?C which is required for drymelting. The genesis of kimberlite can be related to partial meltingof peridotite under conditions of (). Such activities of H2Oresult in melting at depths ranging between 125 and 175 km inthe mantle. This range is within the minimum depth generallyaccepted for the formation of kimberlite.  相似文献   

10.
The so-called 10- phase of the MgO-SiO2-H2O (MSH) system wassynthesized with 100% yields from a 3: 4 MgO/SiO2 gel at fluidpressure of 50 kb and 500 C, but only during runs of up to1 h and with total H2O contents near 50 wt. % in the sealedcapsules. The water contents determined in the run productsindicate a chemical composition Mg3Si4O10(OH)20.65 H2O, whichis different from the composition reported by Bauer & Sclar(1981), which had 1 H2O molecule per talc formula. The 10-phase has a = 5.293(3) , b = 9.194(3) , c = 10.044(3) , ß=96.10(8)its calculated density is pcalc.= 2.672 g/cm3; the refractiveindices measured are nx = 1.554. and nx = 1.574. The compatibilityof mean refractive index, calculated density, and chemical compositionfalls within the category ‘excellent’ of Mandarino(1979). Runs of longer durations and with total H2O again near 50 wt.%, seeded with the less hydrous phase talc with the same Mg/Siratio, show that the 10- phase breaks down in the range 30–70kb, 200–700 C to form more talc. Thus it is not the stablehydrous high-pressure equivalent of talc as reported by Yamamoto& Akimoto (1977), but a metastable phase, which cannot playany role as a natural mineral of the mantle or of subductionzones. If the tie-line forsterite-H2O is stable in the MSH system,as it seems to be for the conditions of our experiments, mostof the hydrous, silica-poor, new high-pressure MSH phases maybe without significance for the Earth, except perhaps phaseA with as yet an ambiguous composition.  相似文献   

11.
The reaction 2 zoisite + CO2 = 3 anorthite + calcite + H2O hasbeen reversed experimentally in cold-seal pressure vessels usingnatural phases and H2O–C02 fluids generated by water-silveroxalate mixtures. Equilibrium has been determined at 5000 50bars, 599 9 °C and 0–075 ± 0–010 XCO2.Extrapolation using the MRK equation of Kerrick & Jacobs(1981) gives an equilibrium curve of negative T–X slopeconsistent with bracketing runs at 500, 550 and 650 °C.The curve agrees only with a new bracket of Nitsch (in Hoschek,1980), and is at higher XCo2 than all other experimental determinationsand at lower XCO2 than those calculated from the thermodynamicdata of Helgeson et al. (1978). Discrepancies are attributedto differences in starting materials and small errors in thethermodynamic properties of the phases. Reaction direction and equilibrium have been determined by observingsurface textures of run products by SEM. Growth and solutiontextures are non-equivalent, permitting unequivocal determinationof reaction direction even where the extent of reaction is small,an advantage over conventional and insensitive XRD methods whichmeasure bulk changes in the charge. Dissolution features ofanorthite and zoisite are defect-related indicating controlby surface reaction, whereas calcite dissolves by both surfacereaction and diffusion controlled processes. Margarite forms in most runs below 585 °C. Textural features,its restriction to the margarite stability field and comparisonwith feldspar solubility data demonstrate it is an equilibriumphase formed by incongruent solubility of anorthite and zoisitein H2O-CO2 fluids. Quench phases formed from the solute areconsequently silica-rich, with implications for metasomaticprocesses in feldspar–epidote–bearing rock and fluidsystems. Absence of margarite from runs with anorthite, zoisiteand calcite in the zoisite stability field is apparently dueto the fast growth rate of zoisite. The full equilibrium assemblageis zoisite–anorthite–calcite–margarite atthese temperatures, and the degeneracy of the model system isunobtainable in experiments, and presumably, in nature.  相似文献   

12.
Volatile Components, Magmas, and Critical Fluids in Upwelling Mantle   总被引：9，自引：2，他引：7  
The phase diagram for lherzolite–CO2–H2O providesa framework for interpreting the distribution of phase assemblagesin the upper mantle with various thermal structures, in differenttectonic settings. Experiments show that at depths >80 km,the near-solidus partial melts from lherzolite–CO2–H2Oare dolomitic, changing through carbonate–silicate liquidswith rising temperatures to mafic liquids; vapor, if it coexists,is aqueous. Experimental data from simple systems suggest thata critical end-point (K) occurs on the mantle solidus at anundetermined depth. Isobaric (T–X) phase diagrams forvolatile-bearing systems with K elucidate the contrasting phaserelationships for lherzolite–CO2–H2O at depths belowand above a critical end-point, arbitrarily placed at 250 km.At levels deeper than K, lherzolite can exist with dolomiticmelt, aqueous vapor, or with critical fluids varying continuouslybetween these end-members. Analyses of fluids in microinclusionsof fibrous diamonds reveal this same range of compositions,supporting the occurrence of a critical end-point. Other evidencefrom diamonds indicates that the minimum depth for this end-pointis 125 km; maximum depth is not constrained. Constructed cross-sectionsshowing diagrammatically the phase fields intersected by upwellingmantle indicate how rising trace melts may influence trace elementconcentrations within a mantle plume. KEY WORDS: mantle solidus; critical end-point; dolomitic magma; diamond inclusions; critical fluids  相似文献   

13.
Carbonate scapolite is a potentially powerful mineral for calculatingCO2 activities in non-calcareous rocks, but an analysis of thethermodynamics and phase equilibria of carbonate scapolite isfirst necessary. This includes an evaluation of Al-Si disorderin meionite, as this has the greatest effect on derived phaserelations. Available experimental data on meionite stability,X-ray diffraction refinements and nuclear magnetic resonancespectra for calcic scapolite do not uniquely constrain the Al-Siordering state of synthetic meionite. However, the data aremost consistent with a high degree of Al-Si disorder and inconsistentwith long-range Al-Si order. An internally consistent thermodynamicdata set was derived and used to calculate P-T and T-XCO2 equilibriainvolving meionite in the CaO-Al2O3-SiO2-CO2-H2O (CASCH) system.The effect of Al-Si disorder is illustrated by calculating thephase equilibria using an ordered, an arbitrary intermediatedisordered, and a completely Al-Si disordered standard statefor meionite. The Gibbs free energy of meionite was calculatedfrom reversals (at 790–815?C, 2–15 kb) on the reaction 3 Anorthite +Calcite =Meionite The fG?m, 298 for each of the standard states is –13 146?6,–13128?8, and –130930kJ/mol, respectively. Becauseof the steep slope of reaction (1) and limited temperature rangeover which it breaks down, meionite used in the experimentsto constrain reaction (1) must possess a limited range of Al-Sidisorder. The P-T slope of reaction (1) increases, and the slopeof meionite decarbonation equilibria changes from positive tonegative in T-XCO2 and P-T space, as a function of increasingAl-Si disorder. Meionite has a wide stability field at highT in T-X space at 5 and 10 kb (PTotal=PFluid), being stableto XCO2=0?06. Meionite alone breaks down to undersaturated gehleniteand/or corundum-bearing assemblages at 5 kb, and to clinozoisiteat 10 kb. The effect of solid solutions on the T-X stabilityof meionite is similar to that of increasing pressure, stabilizingmeionite to lower temperature. Variable Al-Si disorder doesnot significantly affect the upper limit of meionite stabilityin T-XCO2 space. Activity-composition relations for meionitein carbonate scapolite were calculated relative to reaction(1) from data on natural scapolite-plagioclase-calcite assemblages.The extent of departure from ideality varies as a function ofAl-Si disorder. Negative deviations from ideality are indicatedfor natural scapolite solid solutions at T<750?C, based ona disordered Al-Si standard state for meionite. This is likelyto reflect a more ordered Al-Si distribution in natural scapolitescompared with the synthetic endmember standard state. Present address: Department of Earth and Space Sciences, State University of New York, Stony Brook, New York 11794-2100  相似文献   

14.
We have determined the Fe-Mg fractionation between coexistinggarnet and orthopyroxene at 20–45 kb, 975–1400?C,and the effect of iron on alumina solubility in orthopyroxeneat 25 kb, 1200?C, and 20 kb, 975?C in the FMAS system. The equilibriumcompositions were constrained by experiments with crystallinestarting mixtures of garnet and orthopyroxene of known initialcompositions in graphite capsules. All iron was assumed to beFe2+. A mixture of PbO with about 55 mol per cent PbF2 provedvery effective as a flux. The experimental results do not suggest any significant dependenceof KD on Fe/Mg ratio at T 1000?C. The lnKD vs. l/T data havebeen treated in terms of both linear and non-linear thermodynamicfunctional forms, and combined with the garnet mixing modelof Ganguly & Saxena (1984) to develop geothermometric expressionsrelating temperature to KD and Ca and Mn concentrations in garnet. The effect of Fe is similar to that of Ca and Cr3+ in reducingthe alumina solubility in orthopyroxene in equilibrium withgarnet relative to that in the MAS system. Thus, the directapplication of the alumina solubility data in the MAS systemto natural assemblages could lead to significant overestimationof pressure, probably by about 5 kb for the relatively commongarnetlherzolites with about 25 mol per cent Ca+Fe2+ in garnetand about 1 wt. per cent Al2O3 in orthopyroxene.  相似文献   

15.
Fluids and melts have been trapped and analysed in high pressure experiments in the model mantle system MgO-SiO2-H2O at 6 to 10.5 GPa and 900 to 1,200 °C. The fluid/melt traps consisted of a diamond layer that was added to the experimental charge and was separate from the silicate phases. The recovered diamond traps were analysed by laser ablation - ICP - MS. Starting materials were synthetic mixtures of brucite, talc and silica with variable Mg/Si containing 11-31 wt% H2O. Experiments on a serpentine starting composition [Mg3Si2O5(OH)4] result in MgO/SiO2 weight ratios in the subsolidus fluids close to 1 at 6 GPa and close to 2 at 9 GPa. Melt compositions at 6 and 9 GPa have MgO/SiO2 ratios close to that of forsterite. At a single pressure the amount of dissolved silicate in the fluid increases steadily with increasing temperature up to 1,150 °C, where a sudden increase of both SiO2 and MgO is observed. This discrete step marks the solidus, which is more clearly developed at 6 than at 9 GPa. Thus, hydrous melts within the model mantle subsystem Mg2SiO4-Mg2Si2O6-H2O are chemically distinct from aqueous fluids up to at least 9 GPa, corresponding to 300 km depth. Extrapolation of the current data set implies that total convergence between fluid and melt along the solidus probably occurs at 12-13 GPa (~400 km), i.e. close to the Earth's mantle transition zone. Beneath cratons, interactions of hydrous fluids with upper mantle lithologies cause relative silica depletion (olivine enrichment) at depths greater than 200 km and silica (orthopyroxene) enrichment at shallower depths.  相似文献   

16.
Single-phase 2M1 muscovite-paragonite crystalline solutionsin the range 0?00–0?10 and 0?70–1?00 Xms have beensynthesized by hydrothermal treatment of gels of appropriatecompositions at 600–700?C, and 7 to 18 kb PH2O. The molarvolumes of these micas may be expressed as V(J/b?mol) = 13?1845+1?463Xms+0?0160 Xms2–0?1679 Xms3 (?0?005), which translateto a substantial positive excess molar volume of mixing. Na-K ion exchange experiments between presynthesized 2M1 micacrystalline solutions and 2 molal aqueous (Na,K)Cl fluids failedto proceed to completion despite 98 day runs at 500–600?C,6 kb Ptotal. Results of analogous exchange experiments provedencouraging however, when a much finer-grained 1M mica was usedas starting material. Applying the tie line rotation technique,reversal of ion exchange experiments could be achieved in the2-phase fields, not, however, in the 3-phase field of the ms-pg-NaCl-KClreciprocal ternary. Using gels as starting material, reversalexperiments were eventually successful both in the 2-phase andthe 3-phase fields; the results of reversal experiments withinthe two-phase fields being identical to those obtained earlierusing 1M micas. Four isobaric-isothermal sections through the ms-pg-NaCl-KClternary were reversibly determined at 450?C/5 kb, 550?C/6 kb,550?C/15 kb, and 620?C/7 kb. At 450?C, the coexisting mica compositionsin the 3-phase field (2 micas plus 1 fluid) are 0?10 and 0?77Xms, at 550?C they are 0?10 and 0?60 Xms, and finally, at 620?Cthese are 0?12 and 0?51 Xms. To the extent that internal equilibriumwas accomplished between the coexisting micas, these data wouldindicate a wide solvus at 450?C, narrowing gradually with increasingtemperature to 620?C. The critical temperature will be wellin excess of 620?C, although the mica at the critical conditionwill prove to be metastable with respect to the assemblage alkalifeldspars+corundum+H2O. The companion paper by Chatterjee & Flux (1986) presentsa thermodynamic analysis of the above experimental data.  相似文献   

17.
A garnet websterite nodule from the Honolulu volcanic series,Oahu, Hawaii, has been melted in the presence of nearly pureH2O. The solidus is intermediate between that of peridotiteand gabbro. The curve displays a temperature minimum around20 kb reflecting the breakdown of plagioclase. The Iiquidusis between 1130 ?C and 1150 ?C between 10 and 20 kb vapor pressure.Amphibole (pargasitic hornblende) has an extensive stabilityfield, reaching a maximum temperature about 20 ?C below thegarnet websterite liquidus at 15 kb and a maximum pressure of27.5 kb at 950 ?C. The amphibole-out curve intersects the soliduswith a positive slope. Liquids formed by partial melting of garnet websterite are quartz-normativewithin the stability field of amphibole, but become olivine-normative(tholeiitic) with increasing temperature. Amphibole and clinopyroxeneare enriched in Tschermak's molecule at higher temperatures,pargasite content of amphibole increases with increasing pressure. A garnet websterite-rich upper mantle containing modal olivineyields quartz-normative (13–16 per cent), aluminous (21–4wt. per cent A12O3) melts at 17 P 10 kb and in the presenceof nearly pure H2O. However, the presence of amphibole controlsthe liquid composition, a situation not found for liquids formedfrom wet peridotite. In contrast to many basalt liquids, liquidof garnet websterite composition cannot fractionate to andesiteby precipitation of amphibole, as amphibole is not a liquidusphase.  相似文献   

18.
Consideration of available thermodynamic data and the published results of direct experiments relating to (1) formation. of periclase from dolomite and (2) hydration of periclase to brucite, permits the following conclusions to be drawn: (1) At very low partial pressures of CO2 (perhaps of the order of 1 bar) and relatively high partial pressures of water (up to 2000 bars), dolomite can break down directly to brucite and calcite at temperatures above about 400° C, and below temperatures on the brucite dehydration curve. (2) The reaction dolomite calcite + periclase + CO2 in contact metamorphism near granitic bodies is likely to occur only at low partial pressures of CO2 (perhaps 10 or 20 bars); this can be achieved without direct formation of brucite, by maintaining a partial pressure of water of the order of 1000 bars or more. (3) At low CO2 pressures dolomite may re-form in the cooling stages of metamorphism by reaction between calcite, brucite, and CO2 at temperatures below about 400° C.  相似文献   

19.
The Volume and Composition of Melt Generated by Extension of the Lithosphere   总被引：111，自引：2，他引：111  
Calculation of the volume and composition of magma generatedby lithospheric extension requires an accurate mitial geotherm,and knowledge of the variation and composition of the melt fractionas a function of pressure and temperature. The relevant geophysicalobservations are outlined, and geotherms then obtained fromparameterized convective models. Experimental observations whichconstrain the solidus and liquidus at various pressures aredescribed by simple empirical functions. The variation in meltfraction is then parameterized by requiring a variation from0 on the solidus to 1 on the liquidus. The composition of the melts is principally controlled by themelt fraction, though those of FeO, MgO, and SiO2 in additionvary with pressure. Another simple parameterization allows theobserved compositions of major elements in 91 experiments tobe calculated with a mean error of 1.1%, and those of TiO2 andNa2O to 0.3%. These expressions are then used to calculate theexpected compositions of magma produced by adiabatic upwelling.The mean major element composition of the most magnesium-richMORB glasses resemble the mean composition calculated for amantle potential temperature Tp of 1280?C. Adiabatic meltingduring upwelling of mantle of this temperature generates a meltthickness of 7 km. The observed variations of the MgO and TiO2concentrations in a large collection of MORB glass compositionssuggest that extensive low pressure fractional crystallizationoccurs, but that its effect on the concentrations of SiO2, Al2O3,and CaO is small. There is no evidence that normal oceanic crustis produced from magmas containing more than 11% MgO. The mantlepotential temperature within hot rising jets is about 1480?Cand can generate 27 km of magma containing 17% MgO. Extension of the continental lithosphere generates little meltunless ß> 2 and Tp> 1380?C. The melts generatedby larger values of ß or of Tp are alkali basalts,and change to tholeiites as the amount of melting increases.Large quantities of melt can be generated, especially at continentalmargins, where estimates of ß obtained from changesin crustal thickness will in general be too small.  相似文献   

20.
In a global examination of mid-ocean ridge basalt (MORB) glasscompositions, we find that Na8–Fe8–depth variationsdo not support modeling of MORBs as aggregates of melt compositionsgenerated over a large range of temperature and pressure. However,the Na8–Fe8 variations are consistent with the compositionalsystematics of solidus melts in the plagioclase–spinellherzolite transition in the CaO–MgO–Al2O3–SiO2–Na2O–FeO(CMASNF) system. For natural compositions, the P–T rangefor melt extraction is estimated to be 1·2–1·5GPa and 1250–1280°C. This P–T range is a closematch with the maximum P–T conditions for explosive pressure-releasevaporization of carbonate-bearing melts. It is proposed thatfracturing of the lithosphere induces explosive formation andescape of CO2 vapor. This provides the vehicle for extractionof MORBs at a relatively uniform T and P. The upper portionof the CO2-bearing and slightly melted seismic low-velocityzone flows toward the ridge, rises at the ridge axis to lower-lithospheredepths, melts much more extensively during this rise, and releasesMORB melts to the surface driven by explosively escaping CO2vapor. The residue and overlying crust produced by this meltingthen migrate away from the ridge axis as new oceanic lithosphere.The entire process of oceanic lithosphere creation involvesonly the upper 140 km. When lithospheric stresses shift fractureformation to other localities, escape of CO2 ceases, the vehiclefor transporting melt to the surface disappears, and ridgesdie. Inverse correlations of Na8 vs Fe8 for MORB glasses areexplained by mantle heterogeneity, and positive variations superimposedon the inverse variations are consistent with progressive extractionof melts from short, ascending melting columns. The uniformlylow temperatures of MORB extraction are not consistent withthe existence of hot plumes on or close to ocean ridges. Inthis modeling, the southern Atlantic mantle from Bouvet to about26°N is relatively homogeneous, whereas the Atlantic mantlenorth of about 26°N shows significant long-range heterogeneity.The mantle between the Charlie Gibbs and Jan Mayen fracturezones is strongly enriched in FeO/MgO, perhaps by a trappedfragment of basaltic crust. Iceland is explained as the productof this enrichment, not a hot plume. The East Pacific Rise,Galapagos Ridge, Gorda Ridge, and Juan de Fuca Ridge samplemantle that is heterogeneous over short distances. The mantlebeneath the Red Sea is enriched in FeO/MgO relative to the mantlebeneath the northern Indian Ocean.  相似文献   

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