共查询到16条相似文献，搜索用时 15 毫秒
1.
R. Thomas J.D. Webster D. Rhede W. Seifert K. Rickers H.-J. Frster W. Heinrich P. Davidson 《Lithos》2006,91(1-4):137-149
Fractional crystallization of peraluminous F- and H2O-rich granite magmas progressively enriches the remaining melt with volatiles. We show that, at saturation, the melt may separate into two immiscible conjugate melt fractions, one of the fractions shows increasing peraluminosity and the other increasing peralkalinity. These melt fractions also fractionate the incompatible elements to significantly different degrees. Coexisting melt fractions have differing chemical and physical properties and, due to their high density and viscosity contrasts, they will tend to separate readily from each other. Once separated, each melt fraction evolves independently in response to changing T/P/X conditions and further immiscibility events may occur, each generating its own conjugate pair of melt fractions. The strongly peralkaline melt fractions in particular are very reactive and commonly react until equilibrium is attained. Consequently, the peralkaline melt fraction is commonly preserved only in the isolated melt and mineral inclusions.
We demonstrate that the differences between melt fractions that can be seen most clearly in differing melt inclusion compositions are also visible in the composition of the resulting ore-forming and accessory minerals, and are visible on scales from a few micrometers to hundreds of meters. 相似文献
2.
佛冈高分异I型花岗岩的成因:来自Nb-Ta-Zr-Hf等元素的制约 总被引：4，自引：8，他引：4
华南南岭地区发育有大面积的与钨锡成矿相关的侏罗纪花岗岩,然而其中有些花岗岩的成因类型却难以确定。本文以佛冈岩体为例,结合前人已发表数据,对佛冈花岗岩体中Nb、Ta、Zr和Hf等元素的迁移特征及其原理进行探讨,并对佛冈花岗岩的成因类型进行了厘定。随着分异程度增加,佛冈花岗岩Nb和Ta含量增加,Nb/Ta(3.6~15.3)和Zr/Hf(17.3~38.9)比值降低并发生分异。随着Zr含量的降低,佛冈花岗岩的Zr/Hf比值降低,这一特征表明锆石的分离结晶作用使得佛冈花岗岩的Zr/Hf比值分异。Nb/Ta比值分异可能与角闪石和黑云母的分离结晶作用有关。随着Nb/Ta比值降低,Y/Ho比值增加,这一特征表明佛冈花岗岩Nb/Ta比值的分异也和岩浆演化后期的流体有关。佛冈花岗岩不含原生的富铝矿物,为准铝质到弱过铝质岩石。随着分异程度增加,佛冈花岗岩P2O5含量降低,表明它不是S型花岗岩。随着Y/Ho比值增加和Nb/Ta和Zr/Hf比值降低,佛岗花岗岩Ga/Al和Fe OT/Mg O比值增加,从典型I型花岗岩特征演化到类似A型花岗岩的地球化学特征。因此,我们认为佛冈花岗岩不是A型花岗岩而是高分异的I型花岗岩。区域上与成矿相关的流体和花岗质岩浆的相互作用和分离结晶作用,使得华南南岭地区的花岗岩地球化学特征复杂,所以其成因类型也变的难以确定。 相似文献
3.
Voltammetric Determination of High Field‐Strength Elements (Ti,Zr, Hf,Nb, Ta) in Geological Matrices 
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下载免费PDF全文 A voltammetric method for the determination of the high field‐strength elements Ti, Zr, Hf, Nb and Ta by adsorptive stripping of their tartrate complexes is presented. The applicability of the method to geological and metallurgical samples is illustrated by the analysis of certified reference materials (USGS BCR‐2 basalt, BCS‐CRM 388 zircon and Euronorm CRM 579‐1 ferroniobium). Suitable sample preparation techniques, involving fusion with LiBO2 and acidic and basic fluxes, followed by preliminary separation by anion chromatography are described. The method is rapid, affordable and environmentally friendly as it does not require problematic compounds such as hydrofluoric acid or toxic solvents and represents an alternative to more commonly used methods (AAS, ICP‐OES, ICP‐MS). 相似文献
4.
A new, rapid and highly efficient method for the determination of trace amounts of refractory elements (titanium, zirconium, hafnium, vanadium, niobium, tantalum, molybdenum) using micro-column separation/pre-concentration combined with fluorinating electrothermal vaporisation-inductively coupled plasma-mass spectrometry (FETV-ICP-MS) has been developed. In this method, trace amounts of the analytes were selectively adsorbed by a conical micro-column packed with the solid phase extraction material N -benzoyl- N -phenylhydroxylamine loaded on microcrystalline naphthalene at desired pH values. Various factors influencing the separation/pre-concentration, such as pH, sample flow rate and sample volume were studied in detail, and the influences of the organic matrix and the pre-ashing temperature on the determined results were also investigated. Under optimal conditions, the detection limits for Ti, Zr, Hf, V, Nb, Ta and Mo were 0.016, 0.011, 0.010, 0.007, 0.005, 0.006 and 0.003 ng ml−1 , respectively, and the relative standard deviations ranged from 3.3% (Nb) to 9.6% (Hf) ( C = 0.20 ng ml−1 , n = 9). In order to validate the method, the proposed method was applied to the analysis of three certified reference materials (soils GBW07401 and GBW07425; sediment GBW07301a) and the results obtained were in good agreement with the reference values. The method was also successfully applied to the analysis of real seawater samples with satisfactory results. 相似文献
5.
莫河花岗岩的锆石U-Pb和Lu-Hf同位素研究：柴北欧龙布鲁克微陆块始古元古代岩浆作用年龄和地壳演化约束 总被引：1，自引：0，他引：1
欧龙布鲁克微陆块具典型的基底与盖层二元结构,基底自下而上由德令哈杂岩、达肯大坂岩群和万洞沟群三个岩石-构造单元组成.应用LA-ICP-MS测定了德令哈杂岩中的莫河花岗岩体的27个颗锆石的U-Pb同位素成分,其中26颗锆石发生不同程度的放射成因铅同位素丢失,其不一致线上交点年龄为2470＋19/-18 Ma.应用LA-MC-ICP-MS测定了25颗锆石的Hf同位素成分,其中岩浆结晶成因的23颗锆石的Hf（2470 Ma）=0.28129～0.28140,平均值0.28134±0.00003;εHf值的变化范围2.94～6.95,加权平均值4.58＋0.54/-0.76,长英质地壳存留年龄TCDM=2.54～2.75Ga,加权平均值2.66＋0.04/-0.02 Ga.以上数据将该花岗岩的形成年龄约束在2470 Ma,其岩浆来源于地幔物质的部分熔融,指示欧龙布鲁克微陆块在～2.5 Ga的地壳增生事件. 相似文献
6.
高级变质岩中Zr、Hf、Nb、Ta的ICP-MS准确分析 总被引：15，自引：0，他引：15
采用高压密闭溶样ICP－MS研究了片麻岩、榴辉岩等高级变质岩中Nb、Ta、Zr、Hf准确分析方法。实验表明：在温度为190℃时,溶样时间大于36h,Nb、Ta、Zr、Hf可完全溶解,而获得准确的分析结果。但Nb、Ta在稀硝酸介质中的不稳定性会导致分析结果的误差,采用0．1％HF介质的“F^-基体”匹配,可保持Nb、Ta长时间的稳定性。所建立的高压密闭溶样ICP－MS分析方法用于苏鲁－大别地区片麻岩、榴辉岩等高级变质岩的分析,经与XRF及碱熔融ICP－MS方法对比,分析结果具有良好的一致性。 相似文献
7.
The aim of this experimental study was to determine the solubility of cassiterite in natural topaz- and cassiterite-bearing granite melts at temperatures close to the solidus. Profiles of Sn concentrations at glass–crystal (SnO2) interface were determined following the method of (Harrison, T.M., Watson, E.B., 1983. Kinetics of zircon dissolution and zirconium diffusion in granitic melts of variable water content. Contributions to Mineralogy and Petrology 84, 66–72). The cassiterite concentration calculated at the SnO2–glass interface is the SnO2 solubility. Experiments were performed at 700–850 °C and 2 kbar using a natural F-bearing peraluminous granitic melt with 2.8 wt.% normative corundum. Slightly H2O-undersaturated to H2O-saturated melt compositions were chosen in order to minimize the loss of Sn to the noble element capsule walls. At the nickel–nickel oxide assemblage (Ni–NiO) oxygen fugacity buffer, the solubility of cassiterite in melts containing 1.12 wt.% F increases from 0.32 to 1.20 wt.% SnO2 with an increasing temperature from 700 to 850 °C. At the Ni–NiO buffer and a given corundum content, SnO2 solubility increases by 10% to 20% relative to an increase of F from 0 to 1.12 wt.%. SnO2 solubility increases by 20% relative to increasing Cl content from 0 to 0.37 wt.% in synthetic granitic melts at 850 °C. We show that Cl is at least as important as F in controlling SnO2 solubility in evolved peraluminous melts at oxygen fugacities close to the Ni–NiO buffer. In addition to the strong effects of temperature and fO2 on SnO2 solubility, an additional controlling parameter is the amount of excess Al (corundum content). At Ni–NiO and 850 °C, SnO2 solubility increases from 0.47 to 1.10 wt.% SnO2 as the normative corundum content increases from 0.1 to 2.8 wt.%. At oxidizing conditions (Ni–NiO +2 to +3), Sn is mainly incorporated as Sn4+ and the effect of excess Al seems to be significantly weaker than at reducing conditions. 相似文献
8.
The effect of halogens on Zr diffusion and zircon dissolution in hydrous metaluminous granitic melts 总被引：1，自引：0，他引：1
Don R. Baker Aida Conte Carmela Freda Luisa Ottolini 《Contributions to Mineralogy and Petrology》2002,142(6):666-678
Diffusion of Zr and zircon solubility in hydrous, containing approximately 4.5 wt% H2O, metaluminous granitic melts with halogens, either 0.35 wt% Cl (LCl) or 1.2 wt% F (MRF), and in a halogen-free melt (LCO) were measured at 1.0 GPa and temperatures between 1,050 and 1,400 °C in a piston-cylinder apparatus using the zircon dissolution technique. Arrhenius equations for Zr diffusion in each hydrous melt composition are, for LCO with 4.4ǂ.4 wt% H2O: % MathType!MTEF!2!1!+- % feaaeaart1ev0aaatCvAUfKttLearuavP1wzZbItLDhis9wBH5garm % Wu51MyVXgaruWqVvNCPvMCG4uz3bqee0evGueE0jxyaibaieYlf9ir % Veeu0dXdh9vqqj-hEeeu0xXdbba9ev6pc9fs0-rqaqpepmKs4qpepe % I8kaL8kuc9pgc9q8qqaq-dhH6hb9hs0dXdHu6deP0u0-vr0-vr0db8 % meaabaqaciGacaGaaeaabaWaaeaaeaaakeaacqWGebarcqGH9aqpcq % aIYaGmcqGGUaGlcqaI4aaocqaI4aaocqGHXcqScqaIWaamcqGGUaGl % cqaIWaamcqaIZaWmcqWG4baEcqaIXaqmcqaIWaamdaahaaWcbeqaai % abgkHiTiabiIda4aaakiGbcwgaLjabcIha4jabcchaWnaabmaabaWa % aSaaaeaacqGHsislcqaIXaqmcqaI0aancqaIWaamcqGGUaGlcqaIXa % qmcqGHXcqScqaIZaWmcqaIZaWmcqGGUaGlcqaI5aqoaeaacqWGsbGu % cqWGubavaaaacaGLOaGaayzkaaaaaa!571F! D = 2.88 ±0.03x10 - 8 exp( [( - 140.1 ±33.9)/(RT)] )D = 2.88 \pm 0.03x10^{ - 8} \exp \left( {{{ - 140.1 \pm 33.9} \over {RT}}} \right) , for LCl with 4.5ǂ.5 wt% H2O: % MathType!MTEF!2!1!+- % feaaeaart1ev0aaatCvAUfKttLearuavP1wzZbItLDhis9wBH5garm % Wu51MyVXgaruWqVvNCPvMCG4uz3bqee0evGueE0jxyaibaieYlf9ir % Veeu0dXdh9vqqj-hEeeu0xXdbba9ev6pc9fs0-rqaqpepmKs4qpepe % I8kaL8kuc9pgc9q8qqaq-dhH6hb9hs0dXdHu6deP0u0-vr0-vr0db8 % meaabaqaciGacaGaaeaabaWaaeaaeaaakeaacqWGebarcqGH9aqpcq % aIYaGmcqGGUaGlcqaIZaWmcqaIZaWmcqGHXcqScqaIWaamcqGGUaGl % cqaIWaamcqaI1aqncqWG4baEcqaIXaqmcqaIWaamdaahaaWcbeqaai % abgkHiTiabisda0aaakiGbcwgaLjabcIha4jabcchaWnaabmaabaWa % aSaaaeaacqGHsislcqaIYaGmcqaI1aqncqaI0aancqGGUaGlcqaI4a % aocqGHXcqScqaI2aGncqaI0aancqGGUaGlcqaIXaqmaeaacqWGsbGu % cqWGubavaaaacaGLOaGaayzkaaaaaa!5719! D = 2.33 ±0.05x10 - 4 exp( [( - 254.8 ±64.1)/(RT)] )D = 2.33 \pm 0.05x10^{ - 4} \exp \left( {{{ - 254.8 \pm 64.1} \over {RT}}} \right) and for MRF with 4.9ǂ.3 wt% H2O: % MathType!MTEF!2!1!+- % feaaeaart1ev0aaatCvAUfKttLearuavP1wzZbItLDhis9wBH5garm % Wu51MyVXgaruWqVvNCPvMCG4uz3bqee0evGueE0jxyaibaieYlf9ir % Veeu0dXdh9vqqj-hEeeu0xXdbba9ev6pc9fs0-rqaqpepmKs4qpepe % I8kaL8kuc9pgc9q8qqaq-dhH6hb9hs0dXdHu6deP0u0-vr0-vr0db8 % meaabaqaciGacaGaaeaabaWaaeaaeaaakeaacqWGebarcqGH9aqpcq % aIYaGmcqGGUaGlcqaI1aqncqaI0aancqGHXcqScqaIWaamcqGGUaGl % cqaIWaamcqaIZaWmcqWG4baEcqaIXaqmcqaIWaamdaahaaWcbeqaai % abgkHiTiabiwda1aaakiGbcwgaLjabcIha4jabcchaWnaabmaabaWa % aSaaaeaacqGHsislcqaIYaGmcqaIYaGmcqaIZaWmcqGGUaGlcqaI4a % aocqGHXcqScqaIXaqmcqaI1aqncqGGUaGlcqaI1aqnaeaacqWGsbGu % cqWGubavaaaacaGLOaGaayzkaaaaaa!5715! D = 2.54 ±0.03x10 - 5 exp( [( - 223.8 ±15.5)/(RT)] )D = 2.54 \pm 0.03x10^{ - 5} \exp \left( {{{ - 223.8 \pm 15.5} \over {RT}}} \right) . Solubilities determined by the dissolution technique were reversed for LCO +4.5ǂ.5 wt% H2O by crystallization of a Zr-enriched glass of LCO composition at 1,200 and 1,050 °C at 1.0 GPa. The solubility data were used to calculate partition coefficients of Zr between zircon and hydrous melt, which are given by the following expressions: for LCO % MathType!MTEF!2!1!+- % feaaeaart1ev0aaatCvAUfKttLearuavP1wzZbItLDhis9wBH5garm % Wu51MyVXgaruWqVvNCPvMCG4uz3bqee0evGueE0jxyaibaieYlf9ir % Veeu0dXdh9vqqj-hEeeu0xXdbba9ev6pc9fs0-rqaqpepmKs4qpepe % I8kaL8kuc9pgc9q8qqaq-dhH6hb9hs0dXdHu6deP0u0-vr0-vr0db8 % meaabaqaciGacaGaaeaabaWaaeaaeaaakeaacyGGSbaBcqGGUbGBcq % WGebardaqhaaWcbaGaemOwaOLaemOCaihabaGaemOEaONaemyAaKMa % emOCaiNaem4yamMaem4Ba8MaemOBa4Maei4la8IaemyBa0Maemyzau % MaemiBaWMaemiDaqhaaOGaeyypa0JaeGymaeJaeiOla4IaeGOnayJa % eG4mamZaaeWaaeaadaWcaaqaaiabigdaXiabicdaWiabicdaWiabic % daWiabicdaWaqaaiabdsfaubaaaiaawIcacaGLPaaacqGHsislcqaI % 1aqncqGGUaGlcqaI4aaocqaI3aWnaaa!5924! lnDZrzircon/melt = 1.63( [10000/(T)] ) - 5.87\ln D_{Zr}^{zircon/melt} = 1.63\left( {{{10000} \over T}} \right) - 5.87 , for LCl % MathType!MTEF!2!1!+- % feaaeaart1ev0aaatCvAUfKttLearuavP1wzZbItLDhis9wBH5garm % Wu51MyVXgaruWqVvNCPvMCG4uz3bqee0evGueE0jxyaibaieYlf9ir % Veeu0dXdh9vqqj-hEeeu0xXdbba9ev6pc9fs0-rqaqpepmKs4qpepe % I8kaL8kuc9pgc9q8qqaq-dhH6hb9hs0dXdHu6deP0u0-vr0-vr0db8 % meaabaqaciGacaGaaeaabaWaaeaaeaaakeaacyGGSbaBcqGGUbGBcq % WGebardaqhaaWcbaGaemOwaOLaemOCaihabaGaemOEaONaemyAaKMa % emOCaiNaem4yamMaem4Ba8MaemOBa4Maei4la8IaemyBa0Maemyzau % MaemiBaWMaemiDaqhaaOGaeyypa0JaeGymaeJaeiOla4IaeGinaqJa % eG4naCZaaeWaaeaadaWcaaqaaiabigdaXiabicdaWiabicdaWiabic % daWiabicdaWaqaaiabdsfaubaaaiaawIcacaGLPaaacqGHsislcqaI % 0aancqGGUaGlcqaI3aWncqaI1aqnaaa!5920! lnDZrzircon/melt = 1.47( [10000/(T)] ) - 4.75\ln D_{Zr}^{zircon/melt} = 1.47\left( {{{10000} \over T}} \right) - 4.75 and, for MRF by % MathType!MTEF!2!1!+- % feaaeaart1ev0aaatCvAUfKttLearuavP1wzZbItLDhis9wBH5garm % Wu51MyVXgaruWqVvNCPvMCG4uz3bqee0evGueE0jxyaibaieYlf9ir % Veeu0dXdh9vqqj-hEeeu0xXdbba9ev6pc9fs0-rqaqpepmKs4qpepe % I8kaL8kuc9pgc9q8qqaq-dhH6hb9hs0dXdHu6deP0u0-vr0-vr0db8 % meaabaqaciGacaGaaeaabaWaaeaaeaaakeaacyGGSbaBcqGGUbGBcq % WGebardaqhaaWcbaGaemOwaOLaemOCaihabaGaemOEaONaemyAaKMa % emOCaiNaem4yamMaem4Ba8MaemOBa4Maei4la8IaemyBa0Maemyzau % MaemiBaWMaemiDaqhaaOGaeyypa0JaeGymaeJaeiOla4IaeGinaqJa % eG4naCZaaeWaaeaadaWcaaqaaiabigdaXiabicdaWiabicdaWiabic % daWiabicdaWaqaaiabdsfaubaaaiaawIcacaGLPaaacqGHsislcqaI % 0aancqGGUaGlcqaI5aqocqaIXaqmaaa!591C! lnDZrzircon/melt = 1.47( [10000/(T)] ) - 4.91\ln D_{Zr}^{zircon/melt} = 1.47\left( {{{10000} \over T}} \right) - 4.91 . Experiments on the same compositions, but with water contents down to 0.5 wt%, demonstrated reductions in both the diffusion coefficient of Zr and zircon solubility in the melt. The addition of halogens at the concentration levels studied to metaluminous melts has a small effect on either the diffusion of Zr in the melt, or the solubility of zircon at all water concentrations and temperatures investigated. At 800 °C, the calculated diffusion coefficient of Zr is lowest in LCl, 9᎒-17 m2 s-1, and is highest in LCO, 4᎒-15 m2 s-1. Extrapolation of the halogen-free solubility data to a magmatic temperature of 800 °C yields solubilities of approximately one-third of those directly measured in similar compositions, predicted by earlier studies of zircon dissolution and based upon analyses of natural rocks. This discrepancy is attributed to the higher oxygen fugacity of the experiments of this study compared with previous studies and nature, and the effect of oxygen fugacity on the structural role of iron in the melt, which, in turn, affects zircon solubility, but does not significantly affect Zr diffusion. 相似文献
9.
Frank J Millero 《Geochimica et cosmochimica acta》1982,46(1):11-22
The effect of presure on the solubility of minerals in water and seawater can be estimated from In where the volume (ΔV) and compressibility (ΔK) changes at atmospheric pressure (P = 0) are given by Values of the partial molal volume () and compressibilty () in water and seawater have been tabulated for some ions from 0 to 50°C. The compressibility change is quite large (~10 × 10?3 cm3 bar?1 mol?1) for the solubility of most minerals. This large compressibility change accounts for the large differences observed between values of ΔV obtained from linear plots of In Ksp versus P and molal volume data (Macdonald and North, 1974; North, 1974). Calculated values of for the solubility of CaCO3, SrSO4 and CaF2 in water were found to be in good agreement with direct measurements (Macdonald and North, 1974). Similar calculations for the solubility of minerals in seawater are also in good agreement with direct measurements (Ingle, 1975) providing that the surface of the solid phase is not appreciably altered. 相似文献
10.
The effect of compression on noble gas solubility in silicate melts is still badly understood due to a lack of theoretical guidance. In the experimental literature, noble gases dissolving in liquid silicates are found to concentrate almost linearly with increasing pressure up to several tens of kbar, suggesting that Henry’s law could be valid up to very high pressures, although this law stipulates that the gaseous phase in contact with the liquid must be ideal. Recently, new experiments dealing with the dissolution of argon in synthetic and natural silicate melts have pointed out that the evolution of concentration with pressure exhibits a departure from linearity in the 50-100 kbar range, leading either to a levelling off or to a sudden collapse of the argon concentration above 50 kbar. Here, we investigate by means of liquid state physics how volatile species dissolve into silicate melts under pressure. We use a hard sphere model (the reference fluid in liquid state physics) to describe silicate melts and gas at high pressures. One of our main results is that, when pressure increases, the concurrent compaction of gas and melt explains the almost-linear behaviour of the noble gas concentration up to several tens of kbars, before melt compaction dominates and concentration either levels off or decreases gradually in the 50-100 kbar range. In spite of the existence of a quasi-linear regime over a large pressure range, our work disqualifies the use of the Henry law when dealing with high pressures. The implication of these findings to provide an understanding of degassing at mid-ocean ridges is next investigated. Applying our model to the scenario where CO2 vesicle generation occurs in the magma at mantle depths during its ascent from melting regions, we evaluate magma vesicularity as well as noble gas concentrations in the basalt melt and in vesicles as a function of pressure at depth. It is stressed that the variable and usually strong noble gas elemental fractionation observed in mid-ocean ridge basalts can be explained by assuming a sequence of several vesiculation stages interrupted by vesicle loss during magma ascent. 相似文献
11.
12.
阿尔泰南缘阿舍勒盆地泥盆纪火山岩中古老锆石的U-Pb年龄、Hf同位素和稀土元素特征及其地质意义 总被引：5，自引：3，他引：5
阿尔泰造山带南缘发育有NW向斜列的四个泥盆纪海相火山岩沉积盆地,位于北西端的阿舍勒盆地产有阿舍勒大型铜锌矿床,前人对该矿床开展了大量研究,但其容矿火山岩的年龄尚未明确厘定。本文应用LA-ICP-MS锆石U-Pb定年和锆石Hf同位素、微量元素,对阿舍勒铜锌矿区内出露的泥盆纪火山岩进行了研究。由锆石U-Pb定年获得了一组火山岩老锆石谐和年龄为1985±8.9Ma,加权年龄为2005±30Ma,代表了阿尔泰地区前寒武纪结晶基底的形成时代,其Th/U值在0.25～0.90之间,εHf(t)为-1.4～8.5,平均值为3.3;另外一组新锆石年龄为408±8Ma,其εHf(t)为9.3,Th/U值为0.49,具有典型岩浆锆石特征,代表了早泥盆世岩浆活动高峰期一次火山活动时代。老锆石∑REE从最低的1015×10-6变化到最高的3486×10-6,表现为轻稀土亏损,重稀土富集特征;本组锆石不同于正常岩浆锆石的显著特征是部分出现Ce元素负异常。锆石U-Pb年龄、Hf同位素及稀土元素Ce负异常特征综合显示,阿尔泰前寒武纪结晶基底可能形成于Columbia超大陆拼合聚集背景下,其物源来自强还原性地幔物质与氧化性地壳物质的不均匀混合。 相似文献
13.
The effect of alkalis on the solubility of H2O and CO2 in alkali-rich silicate melts was investigated at 500 MPa and 1,250 °C in the systems with H2O/(H2O + CO2) ratio varying from 0 to 1. Using a synthetic analog of phonotephritic magma from Alban Hills (AH1) as a base composition, the Na/(Na + K) ratio was varied from 0.28 (AH1) to 0.60 (AH2) and 0.85 (AH3) at roughly constant total alkali content. The obtained results were compared with the data for shoshonitic and latitic melts having similar total alkali content but different structural characteristics, e.g., NBO/T parameter (the ratio of non-bridging oxygens over tetrahedrally coordinated cations), as those of the AH compositions. Little variation was observed in H2O solubility (melt equilibrated with pure H2O fluid) for the whole compositional range in this study with values ranging between 9.7 and 10.2 wt. As previously shown, the maximum CO2 content in melts equilibrated with CO2-rich fluids increases strongly with the NBO/T from 0.29 wt % for latite (NBO/T = 0.17) to 0.45 wt % for shoshonite (NBO/T = 0.38) to 0.90 wt % for AH2 (NBO/T = 0.55). The highest CO2 contents determined for AH3 and AH1 are 1.18 ± 0.05 wt % and 0.86 ± 0.12 wt %, respectively, indicating that Na is promoting carbonate incorporation stronger than potassium. At near constant NBO/T, CO2 solubility increases from 0.86 ± 0.12 wt % in AH1 [Na/(Na + K)] = 0.28, to 1.18 ± 0.05 wt % in AH3 [Na/(Na + K)] = 0.85, suggesting that Na favors CO2 solubility on an equimolar basis. An empirical equation is proposed to predict the maximum CO2 solubility at 500 MPa and 1,100–1,300 °C in various silicate melts as a function of the NBO/T, (Na + K)/∑cations and Na/(Na + K) parameters: \({\text{wt}}\% \;{\text{CO}}_{2} = - 0.246 + 0.014\exp \left( {6.995 \cdot \frac{\text{NBO}}{T}} \right) + 3.150 \cdot \frac{{{\text{Na}} + {\text{K}}}}{{\varSigma {\text{cations}}}} + 0.222 \cdot \frac{\text{Na}}{{{\text{Na}} + {\text{K}}}}.\) This model is valid for melt compositions with NBO/T between 0.0 and 0.6, (Na + K)/∑cation between 0.08 and 0.36 and Na/(Na + K) ratio from 0.25 to 0.95 at oxygen fugacities around the quartz–fayalite–magnetite buffer and above. 相似文献
14.
Stephen F. Foley Wayne R. Taylor David H. Green 《Contributions to Mineralogy and Petrology》1986,93(1):46-55
Phase relationships in the system kalsilite-forsterite-quartz with fluorine added by direct substitution for oxygen were examined at 28 kb. A large liquidus field for fluorphlogopite exists with approx. 4 wt% F added to the system and the thermal stability of phlogopite is increased by 300° C relative to the water saturated system. Fluorine expands the phase volume of enstatite relative to forsterite so that the peritectic point PHL+EN+FO+L, a model for melting of a phlogopite harzburgite, lies in the silica-undersaturated field. Experimental phlogopites have excess Si which correlates with F content and are Al-deficient. The high Si contents indicate solid solution with an end member intermediate between tri- and di-octahedral micas. Glasses with compositions analogous to partial melts from phlogopite harzburgite were examined by infrared spectroscopy in the mid- and far-IR regions. Results show that fluorine polymerises the melt by bonding with all the network modifying cations K, Mg and Al. At higher F contents, but still less than 1 wt%, tetrahedral KAlO2-groups are complexed by fluorine and removed from the aluminosilicate network simultaneously polymerising and increasing the Si/(Si+Al) ratio of the network. However, when HF rather than F is present, the overall effect will be to depolymerise melts due to the effect of OH released by dissolution of HF. The presence of abundant Si-F bonds is considered unlikely even in silica-rich magmas: the viscosity decrease characteristic of fluorine-bearing melts can be attributed to the formation of fluoride complexes. 相似文献
15.
The landslides in the Three Gorges Reservoir Region,China and the effects of water storage and rain on their stability 总被引：5，自引：0，他引：5
According to the statistics, there were about 1,736 landslides with the total volume of 1.339 × 1011 m3 in the 100 km2 area of upper reaches of the Yangtze River, in which about 94% of landslides are triggered by rain and water storage. Thus,
based investigation of the results of the landslides in this region, this paper completed a systematic study on the effects
of rainfall and water storage on the landslides in the region and found that the distribution of landslides over time and
space are well correlated with the precipitation distribution in this region; landslides are also strictly controlled by the
stratum, geological structure, river valley form, shore type, etc. Meanwhile, the pattern of water table variation of the
three gorges reservoir will do have very serious impacts on the stability of the slopes in this region. All research results
show that water storage and rainfall are the two important inducing factors that can cause a lot of large-scale landslides.
Therefore, some effective control measures for water storage and rainfall should be taken so as to minimize the impacts of
water on the stability of the slopes in the Three Gorges Reservoir Region of Yangtze River, China. 相似文献
16.
干密度和含水率对岩溶地区黄壤抗剪强度的影响——以重庆市南川区木渡河小流域为例 总被引：1，自引：0，他引：1
选择广泛分布于岩溶地区的黄壤,通过对室内三轴剪切试验,测定含水率和干密度交互作用对土壤抗剪强度指标的影响。试验表明:(1)在相同干密度情况下,黄壤粘聚力c随着含水率的增加呈现出先增加后减小的趋势,在相同土壤含水率水平下,粘聚力c随干密度增大而增大;黄壤内摩擦角φ在各干密度条件下均随着含水率增加呈明显减小的趋势,衰减速率基本一致;同一含水率水平下,内摩擦角φ随干密度变化不明显,土壤干密度为1.6g/cm3内摩擦角相对较大。(2)含水率和干密度的交互作用对黄壤粘聚力c有显著影响,粘聚力c在1.3~1.7g/cm3范围内随着干密度的增大而增大,且每一个干密度都有一个特定含水率与之对应,在这样一个交互作用下粘聚力c达到最大。(3)含水率和干密度的交互作用对内摩擦角φ影响相对较小,同一干密度下,其φ值差异不大,随干密度的增大缓慢增大,相对而言,含水率对内摩擦角φ的影响更明显,黄壤内摩擦角φ随含水率的增大呈非线性下降。 相似文献
