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1.
A simple differential thermal analysis (DTA) technique has been developed to study phase relations of various chemical systems at elevated pressures and temperatures. The DTA system has been calibrated against known melting temperatures in the system NaCl-KCl. Isobaric sections of the liquidus in the system NaCl-KCl have been determined at pressures of 1 atmosphere and 500, 1000, 1500, and 2000 bars. Using the least-squares method, the following equation was used to fit the experimental data:
T(°C)=i=06aiXiKCl
where T is the liquidus temperature, XKCl is mole fraction of KCl, and ai (listed below) are the derived empirical constants.
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2.
Self-diffusion of oxygen in adularia, anorthite, albite, oligoclase and labradorite has been measured by isotope exchange of oxygen between natural feldspars and hydrothermal water enriched in 18O. The analysis consisted of measuring the 18O/16O gradient inward from the feldspar surface using an ion microprobe, and fitting a solution of the diffusion equation to the data. Depth of the sputtered hole was measured with an optical interferometer. Linear Arrhenius plots were obtained:
P (bars)aoa1a2a3a4a5a6
1 atm.800.1?334.2781.6?6490.317553.1?17638.46098.3
500813.5?354.9743.3?6011.716406.4?16516.35702.8
1000824.5?406.71446.8?8818.421253.5?20343.76839.4
1500838.6?418.71434.7?8819.021557.9?20908.47123.1
2000848.5?381.51246.9?8605.021785.8?21449.17375.8
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3.
K and Rb distributions between aqueous alkali chloride vapour phase (0.7 molar) and coexisting phlogopites and sanidines have been investigated in the range 500 to 800°C at 2000 kg/cm2 total pressure.Complete solid solution of RbMg3AlSi3O10(OH)2 in KMg3AlSi3O10(OH)2 exists at and above 700°C. At 500°C a possible miscibility gap between approximately 0.2 and 0.6 mole fraction of the Rb end-member is indicated.Only limited solid solution of Rb AlSi3O8 in KAlSi3O8 has been found at all temperatures investigated.Distribution coefficients, expressed as Kd = (Rb/K) in solid/(Rb/K) in vapour, are appreciably temperature-dependent but at each temperature are independent of composition for low Rb end-member mole fractions in the solids. The determined KD values and their approximate Rb end-member mole fraction (XRM) ranges of constancy are summarized as follows: (°C)TKDPhlog/Vap.XRMKDSandi/Vap.Xrm
d0 (cm2/sec)Q (kcal/g-atom O)T(°C)
Adularia (Or98)4.51 × 10?825.6350–700
Albite (Ab97, Ab99)2.31 × 10?921.3350–800
Anorthite (An96)1.39 × 10?726.2350–800
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4.
Oxygen isotope fractionations between wollastonite, diopside, jadeite, hedenbergite and water have been experimentally studied at high pressures (1<- PH2O ≥ 24 kbar) and temperatures (400/dgT <- 800/dgC) using the three-isotope method (Matsuhisa et al., 1978). Initial 18O16O fractionations were made close to equilibrium and initial 17O16O ratios were well removed from equilibrium, allowing accurate determinations of the equilibrium 18O16O fractionations and of the extent of isotopic exchange. Scanning electron microscope and rate studies show that the wollastonite-water and diopside-water exchange reactions occur largely by solution-precipitation (Ostwald Ripening) mechanisms. Equilibrium 18O16O fractionations between water and the minerals wollastonite, diopside, and hedenbergite are in close agreement with one another, whereas significantly more positive fractionations are found for jadeite-water. These isotopic substitution effects can be ascribed to replacement of SiOM bonds (M is a divalent metal cation in octahedral coordination) by higher frequency SiOAl bonds. The fractionations determined in this study can be combined with quartz- and feldspar-water data of Matsuhisa et al. (1979) and revised magnetite-water data of O'NEIL (1963), to provide a coherent set of mineral-pair fractionations satisfactorily represented by straight lines through the origin on a conventional graph of In /ga versus T?2. Mineral-water data, on the other hand, cannot readily be fitted to the simple relationship suggested by Bottinga and Javoy (1973). Coefficients “A” for the mineral-pair fractionations 1000 ln α = A × 106T?2 are:
(°C)TKDPhlog/Vap.XRMKDSanid/Vap.XRM
5000.64 ± 0.110–0.20.17 ± 0.040–0.07
7001.11 ± 0.110–0.20.33 ± 0.040–0.1
8001.28 ± 0.030–0.20.45 ± 0.060–0.1
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5.
E.C. Perry  S.N. Ahmad 《Lithos》1981,14(2):83-92
Oxygen and carbon isotope analyses of samples from three mines in the Krivoy Rog iron formation, Ukranian SSR, are reported here. Maximum and minimum quartz-magnetite fractionation values (ΔQM) and inferred temperature range in degrees centrigrade for each mine are:
AbJdAnDiWoMt
Q0.501.091.592.082.206.11
Ab0.591.091.581.705.61
Jd0.500.991.115.02
An0.490.614.52
Di0.124.03
Wo3.91
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6.
Intercalibration of one intralaboratory and three interlaboratory standards used in 40Ar-39Ar dating has been carried out. In order to provide homogeneous values for 40Ar140K the standards were prepared by careful handpicking. To control the neutron fluence in the Herald Reactor (A.W.R.E.) 16 aliquots of the standards were arranged along 0.6 × 60 cm of a single silica tube. The corrections for all known interferences from K, Ca, Cl were carefully assessed. Two of the hornblende standards, Hb3gr and MMHb-1 appear homogeneous at the 0.1% level while the other two standards, LP-6 and FY12a are not completely homogeneous. The mean values of 40Ar140K when referenced to the previously determined value for Hb3gr (turner et al., 1971) are:
MineΔQMCorresponding temperature
Sevgok9.4 to 14.2475° to 320°C
Ugok10.0 to 12.7450° to 355°C
Annovsky10.5 to 12.6430° to 360°C
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7.
Rb/Sr geochronology on a folded greenstone-granitoid complex in the Agnew area, Western Australia, yields four distinct ages of igneous activity that conform with stratigraphic and intrusive relationships. They are (using λ 87Rb = 1.42 · 10?11a?1, NBS 70A = 522 ppm Rb and 65.3 ppm Sr):
Hb3grhbld.08504 ± .05%(±lσ)1072. m.y.
MMHb-1hbld.03493 ± 05%518.9 m.y.
LP-6biot.007735 ± .13%128.5 m.y.
FY12ahbld.02858 ± .25%435.0 m.y.
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8.
Oxygen isotope fractionations between zoisite and water have been studied at 400–700°C, PH2O = 13.4 kbar, using the three-isotope method described by Matsuhisaet al. (1978) and Matthewset al. (1983a). The zoisite-waier exchange reaction takes place extremely slowly and consequently direct-exchange calibration of equilibrium 18O16O fractionation factors was possible only at 600 and 700°C. Fractionation factors at 400–600°C were determined from samples hydrothermally crystallized from a glass of the anhydrous zoisite composition. At 600°C, both exchange procedures gave identical fractionations within experimental error. Scanning electron microscope studies showed that the zoisite-water exchange reaction occurs largely by solution-precipitation mass-transfer mechanisms. The slow kinetics of zoisite-water exchange may be typical of hydrous silicates, since additional experiments on tremolite-water and chlorite-water exchange also showed very low rates. When the zoisite-water fractionation factors determined in this study are combined with the quartz and albite-water data of Matsuhisaet al. (1979) and the calcite-water data of O'Nellet al. (1969), mineral-pair fractionations are obtained for which the coefficients “A” in the equation 1000 In α = A × 106T?2 are:
Ma87Sr/86Sr initial (IR)
(1) Differentiated gabbro-granophyre from a stratigraphically old (Kathleen Valley) greenstone sequence> 2718 ± 500.7007 ± 0.0004
(2) Voluminous tonalite, the Lawlers Tonalite2652 ± 200.70152 ± 0.00012
2576 ± 140.70218 ± 0.00021
(3) A less voluminous leucogranite, and a large complex pegmatite cutting the Perseverance nickel orebody2588 ± 180.7624 ± 0.0068
(4) Aplitic leucotonalite (very minor volumes but widespread)2474 ± 140.70193 ± 0.00012
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9.
We studied trapping of noble-gases by chromite and carbon: two putative carriers of primordial noble gases in meteorites. Nineteen samples were synthesized in a Ne-Ar-Kr-Xe atmosphere at 440 K to 720 K, by the following reactions: Fe,Cr + 4H2O → (Fe,Cr)3O4 + 4H2 (1) or Fe,Cr + 4CO → (Fe,Cr)3O4 + 4C + carbides (2)The reactant metal films were prepared either by vacuum evaporation of alloy or by thermal decomposition of Fe- and Cr-carbonyls. The products—including Fe3O4, Cr2O3, carbides, and unreacted metal—were partially separated by selective solvents, such as HCl, H2SO4?H3PO4, or HClO4. Samples were characterized by XRD, SEM, and atomic absorption; noble gases were measured by mass spectrometry. Surface areas, as measured by the BET method, were 2 to 100 m2/g.All samples are dominated by an adsorbed noble gas component that is largely released upon heating at ?400°C or slight etching. Elemental abundance patterns show that this component is derived from the highest-pressure noble gas reservoir seen by the sample—atmosphere or synthesis vessel—indicating that desorption or exchange rates at room T are slow on the time scale of our experiments (up to 1 year). Adsorptive capacity is reduced by up to 2 orders of magnitude upon light etching with HClO4 (though the surface area actually doubles in this treatment) and, less drastically, by heating. Apparently some active adsorption sites are destroyed by these treatments. A trapped component (typically 30% of the total) is readily detectable only in samples synthesized at partial pressures close to or greater than atmospheric.Noble gas contents roughly obey Henry's Law, but show only slight, if any, correlations with composition, surface area, or adsorption temperature. (Geometric) mean distribution coefficients for bulk samples and HCl-residues are, in 10?3 cc STP/g atm: Xe (100), Kr (15), Ar (3.5), Ne (0.62). Elemental fractionations are large and variable, but are essentially similar for the adsorbed and trapped components, or for chromite and carbon. They bracket the values for the corresponding meteoritic minerals.
AbCcZo
Q0.500.501.56
Ab0.001.06
Cc1.06
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10.
The Vermilion district of northerneastern Minnesota is a classic example of a lower Precambrian greenstone-granite terrane. It is a complex volcanic-sedimentary pile, characterized by repeated periods of volcanism and the presence of intercalated pyroclastic, volcanoclastic and epiclastic rocks. The volcanic-sedimentary pile is surrounded and intruded by contemporaneous granitic batholiths. Several rock units from the district have been dated by the whole-rock Rb-Sr method. The isochron ages and the corresponding initial Sr87/Sr86 ratios (= I) are:
NeXeArXeKrXe
Geom. mean0.0060.0350.15
Range0.0004-0.030.01-0.20.06-0.4
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11.
12.
Delayed neutron measurements of U and Th in three meteorites yield the following values:
t(in b.y.) ± 2σ1 ± 2σ
Ely Greenstone2.69 ± 0.080.70056 ± 0.00026
Newton Lake Formation2.65 ±0.110.70086 ± 0.00024
Granitic pebbles2.69 ± 0.280.70078 ± 0.00058
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13.
The heat capacities of synthetic pyrope (Mg3Al2Si2O12), grossular (Ca3Al2Si3O12) and a solid solution pyrope60grossular40 (Mg1.8Ca1.2Al2Si3O12) have been measured by adiabatic calorimetry in the temperature range 10–350 K. The samples were crystallized from glasses in a conventional piston-cylinder apparatus.The molar thermophysical properties at 298.15 K (J mol?1 K?1) are:
BruderheimU (ppb)Th(ppb)
Bruderheim14.5 ± 1.0171 ± 65
Peace River11.8 ± 0.796 ± 46
Stannern220 ± 6563 ± 190
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14.
Using the model of fictive ideal components, Gibbs free energies of formation of pyrope and Al2O3-enstatite have been determined from the experimental data on coexisting garnet and orthopyroxene and orthopyroxene and spinel in the temperature range of 1200–1600 K. The negative free energies in kJ/mol are:
CopSo298?So0Ho298?Ho0/T
Pyrope325.31266.2747852
Grossular333.17260.1247660
Py60Gr40328.32268.3247990
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15.
The effect of ionic interactions of the major components of natural waters on the oxidation of Cu(I) and Fe(II) has been examined. The various ion pairs of these metals have been shown to have different rates of oxidation. For Fe(II), the chloride and sulfate ion pairs are not easily oxidized. The measured decrease in the rate constant at a fixed pH in chloride and sulfate solutions agrees very well with the values predicted. The effect of pH (6 to 8) on the oxidation of Fe(II) in water and seawater have been shown to follow the rate equation
-d in [Fe(II)]/dt = k1β1αFe/[H+] + k2β2αFe/[H+]2
where k1 and k2 are the pseudo first order rate constants, β1 and β2 are the hydrolysis constants for Fe(OH)+ and Fe(OH)0. The value of αFE is the fraction of free Fe2+. The value of k1 (2.0 ±0.5 min?1) in water and seawater are similar within experimental error. The value of k2 (1.2 × 105 min?1) in seawater is 28% of its value in water in reasonable agreement with predictions using an ion pairing model.For the oxidation of Cu(I) a rate equation of the form
?d ln [Cu(I)]/dt = k0αCu+ k1β1αCu[Cl]
was found where k0 (14.1 sec?1) and k1 (3.9 sec?1) are the pseudo first order rate constants for the oxidation of Cu+ and CuCl0, β1 is the formation constant for CuCl0 and αCu is the fraction of free Cu+. Thus, unlike the results for Fe(II), Cu(I) chloride complexes have measurable rates of oxidation.  相似文献   

16.
We report Ni, Ga, Ge and Ir concentrations for 193 irons. The compositional trends in groups IIIA and IIIB are redefined, and the suggestion by Wasson and Kimberlin that they represent a single fractionation sequence (group IIIAB) is confirmed. A new group, HIE, is similar in its properties to group IIIA but distinguished by lower Ga/Ni and Ge/Ni ratios, larger bandwidths and the formation of haxonite (Fe, Ni)23C6 in each of its members. A sixth member, Hassi-Jekna, has been added to group IIIC, extending its Ge range up to 70 ppm. The characteristics of these groups can be summarized as follows:
TK12001300140015001600
Pyrope4869.924747.054614.264462.634311.00
Al2O3-enstatite1257.251244.281191.931158.671125.64
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17.
18.
Concentrations of Au, As, Co, Ga, Ge, Ir, Ni and W were determined in the metal of 28 different pallasites plus 6 which are probably paired, to help elucidate their origin. Most divide into two clusters:
GroupStructureNi%Ga(ppm)Ge(ppm)Ir(ppm)
IIIAOm7.1–9.37–2332–470.17–19
IIIBOm8.4–10.516–2127–460.014–0.17
IIICOff-Of10.5–13.011–278.6–700.08–0.6
IIIEOg8.2–8.917–1934–370.05–0.6 The Ge-Ni correlation is positive in IIIA, negative in IIIB and IIIC, and there is no significant correlation in IIIE. San Cristobal is identified as a member of group IAB, thereby extending the Ge and Ni range of this group to 25 ppm and 25 per cent, respectively. Previous reports of wide cooling-rate variations in group IIIAB are not substantiated, and current evidence favors a core over a raisin-bread model for this group. There appears to be no genetic relationship between group IIIAB and either the pallasites or the mesosiderites
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19.
20.
No.Ni (%)Ga (μg/g)Ge (μg/g)Au (μg/g)Fa (mole %)
Main group197.8–11.716–2629–651.7–3.011–13
Eagle Station trio314–164.5–675–1200.8–1.019–20
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