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1.
The Lower Zone of the Eastern Bushveld Complex in the Olifants River Trough   总被引：4，自引：4，他引：4  
The Lower Zone of the Eastern Bushveld Complex in the OlifantsRiver Trough reaches 1584 m in thickness and is divisible intoBasal subzone, Lower Bronzitite, Harzburgite subzone, and UpperBronzitite. The Lower Zone is directly and conformably overlainby the Critical Zone; there is no break between the two. The principal cumulus minerals in the Lower Zone are bronziteand olivine. Chromite is an accessory cumulus mineral in peridotites,especially in the Harzburgite subzone, and cumulus plagioclaseoccurs in two thin units in the Basal subzone. Elsewhere plagioclase,with or without chromian augite, is postcumulus in origin. Electron microprobe analyses show that the range in En and Focontents of bronzite and olivine, respectively, is only a fewper cent over the entire rock sequence. Highest values of bothare found in the Harzburgite subzone. From modal and mineralanalyses the bulk composition of the Lower Zone (wt. per cent)is calculated as SiO2—53.94, TiO2—0.08, Cr2O3—0.55,V2O3—0.01, Al2O3—2.64, NiO—0.09, FeO (totalFe as FeO)—9.62, MnO—0.20, MgO—31.72, CaO—1.48,K2O—0.1, Na2O—0.13. This composition is unlike thatof any magma type, indicating that the Lower Zone is indeeda pile of crystal cumulates. From the data for the Lower Zone, together with available datafor the Critical, Main, and Upper Zones, the average MgO contentof the Eastern Bushveld Complex is calculated as about 13 percent, the Cr content as in excess of 1000 ppm. Even if the Complexformed from a single body of magma, the magma cannot have beentholeiitic, but rather olivine tholeiitic or picritic. An hypothesis of evolution of the Lower Zone is presented. Shiftsin total pressure are inferred to have been a major factor inproducing the succession of rock types and in producing theextraordinarily persistent chromitites of the overlying CriticalZone. It is suggested that the extraordinary richness in chromiteof the Bushveld is related to its formation not from tholeiiticmagma, but from more Mg-rich, chromium-rich magma drawn froma deeper level of the mantle than that which has yielded thetholeiitic basalts.  相似文献   

2.
The Puklen complex of the Mid-Proterozoic Gardar Province, SouthGreenland, consists of various silica-saturated to quartz-bearingsyenites, which are intruded by a peralkaline granite. The primarymafic minerals in the syenites are augite ± olivine +Fe–Ti oxide + amphibole. Ternary feldspar thermometryand phase equilibria among mafic silicates yield T = 950–750°C,aSiO2 = 0·7–1 and an fO2 of 1–3 log unitsbelow the fayalite–magnetite–quartz (FMQ) bufferat 1 kbar. In the granites, the primary mafic minerals are ilmeniteand Li-bearing arfvedsonite, which crystallized at temperaturesbelow 750°C and at fO2 values around the FMQ buffer. Inboth rock types, a secondary post-magmatic assemblage overprintsthe primary magmatic phases. In syenites, primary Ca-bearingminerals are replaced by Na-rich minerals such as aegirine–augiteand albite, resulting in the release of Ca. Accordingly, secondaryminerals include ferro-actinolite, (calcite–siderite)ss,titanite and andradite in equilibrium with the Na-rich minerals.Phase equilibria indicate that formation of these minerals tookplace over a long temperature interval from near-magmatic temperaturesdown to  相似文献   

3.
SEIFERT  F. 《Journal of Petrology》1970,11(1):73-100
The equilibrium temperatures of the reaction muscovite+chlorite+quartz= cordierite+phlogopite+H2O (1) in the pure system K2O—MgO—Al2O2—SiO2—H2Owere found to be 495±10°C at 1 kb PH2O; 525±10°Cat 2 kb; 610±15°C at 5 kb; 635±10°C at6 kb. From intersection of this curve with the lower temperaturestability limit of cordierite close to 645°C, 6.5 kb PH2O,a reaction cordieritc+muscovite = phlogopite+aluminum silicate+quartz+H2O(2) is generated which has a negative slope and passes throughthe points 645°C, 6.5 kb PH2O and 700°C, 5 kb PH2O.On the high-pressure side of this reaction curve cordieriteis restricted to K2O—poor bulk compositions. Application of the experimentally determined phase relationsto more complex natural pelitic rocks suggests that reaction(1) represents maximum temperatures for the disappearance ofchlorite from pelitic assemblages containing muscovite and quartz,whereas reaction (2) gives maximum water pressures for the disappearanceof cordierite from these rocks.  相似文献   

4.
The early augite syenite unit in the 1·13-Ga-old Ilímaussaqintrusive complex, South Greenland, consists of a magmatic assemblageof ternary alkali feldspar + fayalitic olivine + augite + titanomagnetite+ apatite + baddeleyite ± nepheline ± quartz ±ilmenite ± zircon. Feldspar, nepheline and QUILF thermometryyield T = 1000–700°C, at P = 1 kbar, which is derivedfrom fluid inclusion data from other parts of the complex. Ternaryfeldspar was the first major liquidus phase. It crystallizedat temperatures between 950 and 1000°C from a homogeneousmagma with aSiO2 = 0·8 and fO2 about 1·5–2log units below the fayalite–magnetite–quartz (FMQ)buffer. Later, closed system fractionation produced nepheline-bearingassemblages with aSiO2 = 0·4 and log fO2 = FMQ –3 to FMQ – 5. Assimilation of wall rocks produced localvariations of melt composition. Four traverses through the unitwere sampled parallel to the assumed direction of crystallization.They exhibit significant differences in their mineral assemblagesand compositions. The chemical zoning and calculated intensiveparameters of four sample suites reflect both closed systemfractional crystallization and local assimilation of wall rocks. KEY WORDS: alkaline magmatism; assimilation; fractionation; redox equilibria; QUILF  相似文献   

5.
Experiments in the quartz-saturated part of the system KFMASHunder fO2 conditions of the haematite–magnetite bufferand using bulk compositions with XMg of 0·81, 0·72,0·53 define the stability limits of several mineral assemblageswithin the P–T field 9–12 kbar, 850–1100°C.The stability limits of the mineral assemblages orthopyroxene+ spinel + cordierite ± sapphirine, orthopyroxene + garnet+ sapphirine, sapphirine + cordierite + orthopyroxene and garnet+ orthopyroxene + spinel have been delineated on the basis ofP–T and T–X pseudosections. Sapphirine did not appearin the bulk composition of XMg = 0·53. A partial petrogeneticgrid applicable to high Mg–Al granulites metamorphosedat high fO2, developed in our earlier work, was extended tohigher pressures. The experimental results were successfullyapplied to several high-grade terranes to estimate P–Tconditions and retrograde P–T trajectories. KEY WORDS: KFMASH equilibria; experimental petrogenetic grid at high fO2  相似文献   

6.
The aluminous pyroxene, fassaite, occurs in two small tabularbodies within mafic plutonites of the Boulder Batholith nearits north-east margin twelve miles east of Helena, Montana.First described by Knopf & Lee (1957), the bodies are contact-metasomatizedlimestone septa, now magnesian-tactites, consisting chieflyof fassaite, spinel, garnet, vesuvianite, and clintonite. Lesscommon minerals include pargasite, diopside, wollastonite, sphene,perovskite, anorthite, forsterite, calcite and chlorite. Sometwenty-five microprobe analyses of the fassaite show it is variablein composition and largely consists of the components CaMgSi2O6(53–83 per cent), CaAl2SiO6 (7–25 per cent), CaFeAlSiO6(8–28 per cent), and CaTiAl2O6 (0–7 per cent). Thestoichiometry generally requires that most of the iron is ferric,consistent with Mössbauer data taken on a typical sample.If fassaite analyses from these and other contact metamorphicrocks are plotted on a triangular diagram with Ca(Mg,Fe)Si2O6,CaAl2SiO6 and CaFeAlSiO6 as end-members, the distribution ofpoints offers no positive evidence for a solvus gap betweenfassaite and diopside as proposed by Ginzburg (1969). The mostaluminous fassaites occur with spinel-clintonite ± grossularand have 25 per cent of the Si replaced by Al, making them truepolymorphs of a garnet (i.e. Gr42And23Pp35). No unusual cationordering is detected in these fassaites by single-crystal X-rayphotographs or Mössbauer measurements. Smede's (1966) estimate of 3–4 km of stratigraphic coverfor the Boulder Batholith indicates pressures of approximately1 kb, in agreement with the occurrence of andalusite + K-feldsparin a hornfels at the Kokaruda Ranch complex. The partial assemblagesof grossular, epidote, perovskite, anorthite-wollastonite, anorthite-calcite,and fassaite-calcite require XCO2 = 0·12 ± 0·08and T = 570 ± 10 °C at these pressures. These pressuresand temperatures place this occurrence in the upper portionsof the hornblende-hornfels facies after Turner (1968), althoughthe low pressures and water-rich fluids permit assemblages (wollastonite,calcite-forsterite-diopside) that Turner lists as characteristicof the pyroxene-hornfels facies.  相似文献   

7.
An internally consistent set of activity-composition relationsfor Fe-Mg-Ca garnets constrained from calorimetric and phaseequilibrium experiments provides the basis for refining theorthopyroxene-garnet thermometer and the orthopyroxene-garnet-plagioclase-quartzbarometer based on the equilibria FeSiO3 + 1/3Mg3Al2Si3O12 = MgSiO3 + 1/3Fe3Al2Si3O12 (A) Mg2Si2O6 + CaAl2Si2O8 = 2/3 Mg3Al2Si3O12 + 1/3 Ca3Al2Si3O12+ SiO2 (B) Fe2Si2O6 + CaAl2Si2O8 = 2/3 Fe3Al2Si3O12 + 1/3 Ca3Al2Si3O12+ SiO2. (C) The major modification arises from better constrained valuesof mixing parameters for the pyrope-almandine binary. Thermodynamicanalysis of reversed experimental data on Fe-Mg partioning betweenorthopyroxene and garnet (Kawasaki & Matsui, 1983; Lee &Ganguly, 1988), when combined with the enthalpy of solutiondata for the pyrope-almandine binary (Geiger et al.t 1987),yields and AGIT of the exchange reaction as cal in the temperaturerange 1248–1573 K. The retrieved data, combined with the known thermochemical parametersfor the pyrope-grossular and almandine-grossular binaries andcomplementary phase equilibrium data, have been used to estimatetemperatures from equilibrium (A) and pressures from equilibria(B) and (C). The geothermometer registers temperatures higherby 70–100C than those obtained from Harley's (1984) formulationand 20–40?C lower than those from Lee & Ganguly's(1988) formulation for granulite grade rocks; the scatter inestimated temperatures for all areas is lower when comparedwith the other two formulations. The estimated pressures from(B) and (C) are reasonable for granulite grade rocks in thepressure range 3.0–12.0 kb and agree, in most cases, within? 1000'b. The smaller scatter in the computed temperatures and convergenceof calculated pressure values support the claim that the formulationspresented here represent improved versions of the orthopyroxene-garnetgeothermometer and the orthopyroxene-garnet-plagioclase-quartzgeobarometer.  相似文献   

8.
Garnet-bearing assemblages of K-rich and K-poor metapelitesfrom the Ilesha Schist belt, SW Nigeria, are investigated. K-richsamples contain the assemblages (A) garnet–staurolite–muscovite–chlorite–magnetite,(B) andalusite–garnet–staurolite–muscovite–chlorite–magnetiteand (C) sillimanite–andalusite–garnet–muscovite–chlorite–magnetite.K-poor samples contain the assemblages (D) garnet–staurolite–cordierite–chloriteand (E) garnet–cordierite–chlorite ± staurolite.All assemblages contain quartz, plagioclase, biotite and ilmenite.P–T pseudosections calculated in the system CaO–Na2O–K2O–TiO2–MnO–FeO–MgO–Al2O3–SiO2 –H2O ± O2 suggest peak metamorphismat 590 ± 20°C at 5 ± 0·5 kbar, followedby retrogression to 550°C at 3·0 kbar, in agreementwith field evidence, domain assemblages, mineral compositions,modes and geothermobarometry. The absence of compositional zonationshows that garnet in all investigated rocks nucleated and grewat constant P–T–X in equilibrium with associatedminerals on the thin-section scale. However, the garnet-in reactiondid not begin until the establishment of a significant temperatureoverstep of  相似文献   

9.
Using an internally consistent thermodynamic dataset and updatedmodels of activity–composition relation for solid solutions,petrogenetic grids in the system NKFMASH (Na2O–K2O–FeO–MgO–Al2O3–SiO2–H2O)and the subsystems NKMASH and NKFASH have been calculated withthe software THERMOCALC 3.1 in the P–T range 5–36kbar and 400–810°C, involving garnet, chloritoid,biotite, carpholite, talc, chlorite, kyanite/sillimanite, staurolite,phengite, paragonite, albite, glaucophane, jadeite, with quartz/coesiteand H2O in excess. These grids, together with calculated AFMcompatibility diagrams and P–T pseudosections, are shownto be powerful tools for delineating the phase equilibria andP–T conditions of Na-bearing pelitic assemblages for avariety of bulk compositions from high-P terranes around theworld. These calculated equilibria are in good agreement withpetrological studies. Moreover, contours of the calculated phengiteSi isopleths in P–T pseudosections for different bulkcompositions confirm that phengite barometry is highly dependenton mineral assemblage. KEY WORDS: phase relations; HP metapelite; NKFMASH; THERMOCALC; phengite geobarometry  相似文献   

10.
Phase relations for the bulk compositions 3CaO·2FeOx·3SiO2+excessH2O and CaO·FeOx·2SiO2+excess H2O were determinedusing conventional hydrothermal techniques with solid phaseoxygen buffers to control fO2. Andradite, Ca3Fe3+2Si3O12, synthesized above 550 °C hasan average unit cell edge, ao, of 12.055±0.001 Å,and an index of refraction, n, of 1.887±0.003. Belowthis temperature, ao increases whereas n decreases, indicatingthe formation of a member of the andradite-hydroandradite solidsolution. At 2000 bars Pfluid andradite is stable above an fO2of 1015 bar at 800 °C and 10-32 bar at 400 °C. At lowerfO2 andradite+fluid gives way at successively lower temperaturesto the condensed assemblages magnetite+wollastonite, kirschsteinite(CaFe2+SiO4)+ wollastonite and kirschsteinite+xonotlite (Ca6Si6O17(OH)2). Synthetic hedenbergite, CaFe2+Si2O6, has average unit cell dimensionsof ao = 9.857± 0.004 Å, bo = 9.033±0.002Å, co = 5.254±0.002 Å and ß = 104.82°±0.03°,and refractive indices of n = 1.731±0.003 and n = 1.755±0.005.At 2000 bars Pfiuid, hedenbergite is stable below an fO2 of10-13 bar at 800 °C and 10-28 bar at 400 °C. Above thesefO2 values, hedenbergite+O2 breaks down to andradite+magnetite+quartz. The mineral pair andradite +hedenbergite thus limit the fO2range possible for their joint formation under equilibrium conditions. The hydration of wollastonite to xonotlite occurs at much lowertemperatures than previous experimental work indicated. A tentativehigh temperature limit for this reaction is set at 185°±15°C and 5000±25 bars and 210°±15 °Cand 2000±20 bars. Inasmuch as the growth of xonotlitefrom wollastonite + H2O was never accomplished, this high temperaturelimit does not represent an equilibrium univariant curve. Nine phases were encountered in the study of andradite and hedenbergite.They are andradite, hedenbergite, magnetite, wollastonite, kirschsteinite,xonotlite, quartz, ilvaite, and vapor (fluid). An invariantpoint analysis using the method of Schreinemakers shows thetopologic relations of the reactions involved. The resultinggrid can be used to interpret natural occurrences.  相似文献   

11.
The redox state of sillimanite zone (650–700°C, 5–6kbar) metasediments of the Barrovian type area, Scotland, wasinvestigated using estimates of metamorphic oxygen fugacity(fO2), sulfur fugacity (fS2), and fluid chemistry based on newdeterminations of mineral and rock compositions from 33 samples.A total of 94% of the samples lack graphite, contain both ilmenite–hematitesolid solutions (RHOMOX) and magnetite, and had metamorphicfO2 about 2 log10 units above the quartz–fayalite–magnetite(QFM) buffer. The regional variation in metamorphic fO2 forthese rocks was minimal, about ±0·3 log10 units,reflecting either a protolith that was homogeneous with respectto redox state, or an initially variable protolith whose redoxstate was homogenized by metamorphic fluid–rock interaction.RHOMOX inclusions in garnet porphyroblasts that become richerin ilmenite from the interior to the edge of the host porphyroblastsuggest that at least some syn-metamorphic reduction of rockoccurred. Significant variations in bulk-rock oxidation ratio(OR) that are probably inherited from sedimentary protolithsare found from one layer to the next; OR ranges mostly between  相似文献   

12.
We have investigated the stability and composition of potassiumamphibole and its high-pressure breakdown product phase X insynthetic peralkaline and subalkaline KNCMASH (K2O–Na2O–CaO–MgO–Al2O3–SiO2–H2O)and natural KLB-1 peridotite bulk compositions between 10 and23 GPa at 800–1800°C. In the KNCMASH system, potassiumamphibole reaches its upper pressure stability limit at 13–15GPa at  相似文献   

13.
Alpine-type peridotites and associated pyroxenites are foundas lenses in the continental crust in many different orogens.The reconstruction of the pressure–temperature (P–T)evolution of these rocks is, however, difficult or even impossible.With geothermobarometry, usually one point on the overall P–Tpath can be obtained. To use the different mineral assemblagesobserved in ultramafic rocks as P–T indicators, quantitativeP–T phase diagrams are required. This study presents newcalculated phase diagrams for peridotitic and pyroxenitic rocksin the model systems CaO–MgO–Al2O3–SiO2–H2O(CMASH) and Na2O–CaO–MgO–Al2O3–SiO2–H2O(NCMASH), which include the respective solid solutions as continuousexchange vectors. These phase diagrams represent applicablepetrogenetic grids for peridotite and pyroxenite. On the basisof these general petrogenetic grids, phase diagrams for particularperidotite and pyroxenite bulk compositions are constructed.In an example of pyroxenite from the Shackleton Range, Antarctica,the different observed mineral assemblages are reflected bythe phase diagrams. For these rocks, a high-pressure metamorphicstage around 18 kbar and an anticlockwise P–T evolution,not recognized previously, can be inferred. KEY WORDS: Antarctic; high-pressure metamorphism; peridotite; phase diagrams; pyroxenite  相似文献   

14.
Synthesis and Stability Relations of Epidote, Ca2Al2FeSi3O12 (OH)   总被引：2，自引：0，他引：2  
LIOU  J. G. 《Journal of Petrology》1973,14(3):381-413
Hydrothermal investigation of the bulk composition 2CaO·Al2O3·l/2Fe2O2·3SiO2+excessH2O (Ps 33 +excess H2O) has been conducted using conventionalapparatus and solid oxygen buffer techniques. Coarse-grainedepidotes (over 150 microns in some cases) were readily synthesizedfrom oxide mixtures with a 98 per cent yield as well as fromtheir high temperature equivalents at 600–700 °C and5 kb Pfluid and over a range of oxygen fugacities. Electronmicroprobe analyses show that maximum Fe+3 content of syntheticepidotes varies as a function of fo2. Epidote is most iron-rich(Ps 33 ± 2) at high (HM and CCO) oxygen buffers and becomesprogressively more aluminous (Ps 25 ± 3) with decreasingfo2 values and temperatures. Such variation is consistent withthe change of refractive indices and cell dimensions. The meanrefractive indices and cell dimensions for synthetic epidote(Ps 33) are N = 1.745 ± 0.005, N = l.786±0.005,a = 8.920±0.005 Å, b = 5.645±0.004 Å,c = 10.190 ű0.006 Å, and ß = 115°31'±4' and for epidote (Ps 25) are N = 1.735±0.005,N = 1.775±0.005, a = 8.891±0.005 Å, b =5.625±0.004 Å, c = 10.177±0.006 Å,and ß = 115° 30'±3'. Mössbauer spectraindicate synthetic epidotes are relatively disordered. Garnets of intermediate composition in the grossular-andraditeseries were synthesized and the cell dimensions and refractiveindices vary linearly with composition. With successive decreasein fo2, garnet synthesized on the Ps 33 bulk composition movestoward the grossular end member with simultaneously increasingalmandine component; concomitantly the hercynite component ofthe coexistent magnetite increases. The fo2-T-Pfluid relations were determined by employing mineralmixtures of synthetic epidote and its high temperature equivalentin subequal proportions. Equilibrium was demonstrated for thereactions (1) epidote (Ps 33) = anorthite+grandite+FeOx+quartz+ fluid, and (2) epidote (Ps 25) (+quartz) = garnet38+anorthite+magnetitc+fluid.With fo2 defined by the HM buffer, epidote (Ps 33) is stableup to 748 °C, 5 kb, 678 °C, 3 kb, and 635 °C, 2kb Pfluid. With fo2 defined by the NNO buffer, the epidote (Ps25) high temperature stability limit is reduced about 100 °Cat 5kb Pfluid. At slightly lower fo2, than defined by the QFMbuffer, epidote is not stable at any temperatures; the assemblagehedenbergite+anorthite+garnet38+fluid replaces epidote in thepresence of excess quartz. Combined with previously determined equilibria for prehnite,andradite, and hedenbergite, isobaric fo,-T relations were furtherinvestigated by chemographic analysis interrelating the phasesprehnite, epidote, grandite, hedenbergite, wollastonite, anorthite,and magnetite in the system CaO-Fe2O3-Al2O3-SiO2-H20. Such analysisallowed the construction of a semi-quantitative petrogeneticgrid applicable to natural parageneses in low µCO2 environments,and the delineation of the low temperature stability limit ofepidote as a function of fo2. Enlargement of the epidote stabilityrange toward both high and low temperatures with increasingfo2, is consistent with widespread occurrences of epidote inlow- and mediumgrade metamorphic rocks.  相似文献   

15.
The solubility of sulfur as S2– has been experimentallydetermined for 19 silicate melt compositions in the system CaO–MgO–Al2O3–SiO2(CMAS)± TiO2 ± FeO, at 1400°C and 1 bar, using CO–CO2–SO2gas mixtures to vary oxygen fugacity (fO2) and sulfur fugacity(fS2). For all compositions, the S solubility is confirmed tobe proportional to (fS2/fO2)1/2, allowing the definition ofthe sulfide capacity (CS) of a silicate melt as CS = [S](fO2/fS2)1/2.Additional experiments covering over 150 melt compositions,including some with Na and K, were then used to determine CSas a function of melt composition at 1400°C. The resultswere fitted to the equation  相似文献   

16.
The pressure-temperature-compositional (P-T-X) dependence ofthe solubility of Al2O3 in orthopyroxene coexisting with garnethas been experimentally determined in the P-T range 5–30kilobars and 800–1200 ?C in the system FeO—MgO—Al2O3—SiO2(FMAS). These results have been extended into the CaO—FeO—MgO—Al2O3—SiO2(CFMAS) system in a further set of experiments designed to determinethe effect of the calcium content of garnet on the Al2O3 contentsof coexisting orthopyroxene at near-constant Mg/(Mg + Fe). Startingmaterials were mainly glasses of differing Mg/(Mg + Fe) or Ca/(Ca+ Mg + Fe) values, seeded with garnet and orthopyroxene of knowncomposition, but mineral mixes were also used to demonstratereversible equilibrium. Experiments were performed in a piston-cylinderapparatus using a talc/pyrex medium. Measured orthopyroxene and corrected garnet compositions werefitted by multiple and stepwise regression techniques to anequilibrium relation in the FMAS system, yielding best-fit,model-dependent parameters Goy= –5436 + 2.45T cal mol–1,and WM1FeA1= –920 cal mol–1. The volume change ofreaction, Vo, the entropy change, So970 and the enthalpy changeHo1,970, were calculated from the MAS system data of Perkinset al. (1981) and available heat capacity data for the phases.Data from CFMAS experiments were fitted to an expanded equilibriumrelation to give an estimate of the term WgaCaMg = 1900 ? 400cal/mole cation, using the other parametric values already obtainedin FMAS. The experimental data allow the development of a arnet-orthopyroxenegeobarometer applicable in FMAS and CFMAS: where This geobarometer is applicable to both pelitic and metabasicgranulites containing garnet orthopyroxene, and to garnet peridoditeand garnet pyroxenite assemblages found as xenoliths in diatremesor in peridotite massifs. It is limited, however, by the necessityof an independent temperature estimate, by errors associatedwith analysis of low Al2O3 contents in orthopyroxenes in high-pressureor low-temperature parageneses, and by uncertainties in thecomposition of garnet in equilibrium with orthopyroxene. Ananalysis of errors associated with this formulation of the geobarometersuggests that it is subject to great uncertainty at low pressuresand for Fe-rich compositions. The results of application ofthis geobarometer to natural assemblages are presented in acompanion paper.  相似文献   

17.
We apply an oxygen barometer based on the Fe content of CaTiO3perovskite to estimate the oxygen fugacity (fO2) during thecrystallization and emplacement of kimberlites in differenteruptive phases of a single pipe, or between different pipes,clusters or provinces. Mineral chemical data for perovskitewere compiled from the literature and obtained in our detailedstudy of perovskites from 11 kimberlites at Somerset Islandand Lac de Gras, Canada. Perovskite compositions in kimberlitesrecord a range in fO2 of many orders of magnitude from NNO–5to NNO+6 [where log fO2 is given relative to the nickel–nickeloxide (NNO) buffer]. The range of fO2 recorded by differentparageneses of perovskite within a single pipe can vary up tothree orders of magnitude with trends toward both oxidationand reduction during crystallization. Kimberlites record someof the greatest ranges, and the highest known fO2 conditionsfor any terrestrial magma. This is attributed to the presenceof deep and oxidized source regions and the variable interplayof ferric–ferrous vs carbon–fluid equilibria duringascent of kimberlite magmas. Three kimberlite pipes from theLac de Gras field show that higher fO2 values correlate withhigher proportions of more resorbed diamonds, suggesting thatthis variable has a measurable effect on the physical propertiesof diamonds in a pipe. KEY WORDS: kimberlites; oxygen fugacity; perovskite; diamond; redox; mantle  相似文献   

18.
Fe–Mg exchange is the most important solid solution involvedin partial melting of spinel lherzolite, and the system CaO–MgO–Al2O3–SiO2–FeO(CMASF) is ideally suited to explore this type of exchange duringmantle melting. Also, if primary mid-ocean ridge basalts arelargely generated in the spinel lherzolite stability field bynear-fractional fusion, then Na and other highly incompatibleelements will early on become depleted in the source, and themelting behaviour of mantle lherzolite should resemble the meltingbehaviour of simplified lherzolite in the CMASF system. We havedetermined the isobarically univariant melting relations ofthe lherzolite phase assemblage in the CMASF system in the 0·7–2·8GPa pressure range. Isobarically, for every 1 wt % increasein the FeO content of the melt in equilibrium with the lherzolitephase assemblage, the equilibrium temperature is lower by about3–5°C. Relative to the solidus of model lherzolitein the CaO–MgO–Al2O3–SiO2 system, melt compositionsin the CMASF system are displaced slightly towards the alkalicside of the basalt tetrahedron. The transition on the solidusfrom spinel to plagioclase lherzolite has a positive Clapeyronslope with the spinel lherzolite assemblage on the high-temperatureside, and has an almost identical position in P–T spaceto the comparable transition in the CaO–MgO–Al2O3–SiO2–Na2O(CMASN) system. When the compositions of all phases are describedmathematically and used to model the generation of primary basalts,temperature and melt composition changes are small as percentmelting increases. More specifically, 10% melting takes placeover 1·5–2°C, melt compositions are relativelyinsensitive to the degree of melting and bulk composition, andequilibrium and near-fractional melting yield similar melt compositions.FeO and MgO are the oxides that exhibit the greatest changein the melt with degree of melting and bulk composition. Theamount of FeO decreases with increasing degree of melting, whereasthe amount of MgO increases. The coefficients for Fe–Mgexchange between the coexisting crystalline phases and melt,KdFe–Mgxl–liq, show a relatively simple and predictablebehaviour with pressure and temperature: the coefficients forolivine and spinel do not show significant dependence on temperature,whereas the coefficients for orthopyroxene and clinopyroxeneincrease with pressure and temperature. When melting of lherzoliteis modeled in the CMASF system, a strong linear correlationis observed between the mg-number of the lherzolite and themg-number of the near-solidus melts. Comparison with meltingin the CMASN system indicates that Na2O has a strong effecton lherzolite melting behaviour only at small degrees of melting. KEY WORDS: CMASF; lherzolite solidus; mantle melting  相似文献   

19.
Petrogenetic grids in the system NCKFMASH (Na2O–CaO–K2O–FeO–MgO–Al2O3–SiO2–H2O)and the subsystems NCKMASH and NCKFASH calculated with the softwareTHERMOCALC 3.1 are presented for the P–T range 7–30kbar and 450–680°C, for assemblages involving garnet,chloritoid, biotite, carpholite, talc, chlorite, kyanite, staurolite,paragonite, glaucophane, jadeite, omphacite, diopsidic pyroxene,plagioclase, zoisite and lawsonite, with phengite, quartz/coesiteand H2O in excess. These grids, together with calculated compatibilitydiagrams and P–T and T–XCa and P–XCa pseudosectionsfor different bulk-rock compositions, show that incorporationof Ca into the NKFMASH system leads to many of the NKFMASH invariantequilibria moving to lower pressure and/or lower temperature,which results, in most cases, in the stability of jadeite andgarnet being enlarged, but in the reduction of stability ofglaucophane, plagioclase and AFM phases. The effect of Ca onthe stability of paragonite is dependent on mineral assemblageat different P–T conditions. The calculated NCKFMASH diagramsare powerful in delineating the phase equilibria and P–Tconditions of natural pelitic assemblages. Moreover, contoursof the calculated phengite Si isopleths in P–T and P–XCapseudosections confirm that phengite barometry in NCKFMASH isstrongly dependent on mineral assemblage. KEY WORDS: phase relations; metapelites; NCKFMASH; THERMOCALC; phengite geobarometry  相似文献   

20.
Metapelitic rock samples from the NE Shackleton Range, Antarctica,include garnet with contrasting zonation patterns and two agespectra. Garnet porphyroblasts in K-rich kyanite–sillimanite–staurolite–garnet–muscovite–biotite schistsfrom Lord Nunatak show prograde growth zonation, and give Sm–Ndgarnet, U–Pb monazite and Rb–Sr muscovite ages of518 ± 5, 514 ± 1 and 499 ± 12 Ma, respectively.Geothermobarometry and P–T pseudo-section calculationsin the model system CaO–Na2O–K2O– TiO2–MnO–FeO–MgO–Al2O3–SiO2–H2Oare consistent with garnet growth during prograde heating from540°C/7 kbar to 650°C/7·5 kbar, and partial resorptionduring a subsequent P–T decrease to <650°C at <6kbar. All data indicate that rocks from Lord Nunatak were affectedby a single orogenic cycle. In contrast, garnet porphyroblastsin K-poor kyanite–sillimanite– staurolite–garnet–cordierite–biotite-schistsfrom Meade Nunatak show two growth stages and diffusion-controlledzonation. Two distinct age groups were obtained. Laser ablationplasma ionization multicollector mass spectrometry in situ analysesof monazite, completely enclosed by a first garnet generation,yield ages of c. 1700 Ma, whereas monazite grains in open garnetfractures and in most matrix domains give c. 500 Ma. Both agegroups are also obtained by U–Pb thermal ionization massspectrometry analyses of matrix monazite and zircon, which fallon a discordia with lower and upper intercepts at 502 ±1 and 1686 ± 2 Ma, respectively. Sm–Nd garnet datingyields an age of 1571 ± 40 Ma and Rb–Sr biotiteanalyses give an age of 504 ± 1 Ma. Integrated geochronologicaland petrological data provide evidence that rocks from MeadeNunatak underwent a polymetamorphic Barrovian-type metamorphism:(1) garnet 1 growth and subsequent diffusive garnet annealingbetween 1700 and 1570 Ma; (2) garnet 2 growth during the RossOrogeny at c. 500 Ma. During the final orogenic event the rocksexperienced peak P–T conditions of about 650°C/7·0kbar and a retrograde stage at c. 575°C/4·0 kbar. KEY WORDS: garnet microtexture; P–T pseudosection; geochronology; polymetamorphism; Shackleton Range; Antarctica  相似文献   

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