共查询到19条相似文献，搜索用时 276 毫秒
1.
矿物氧扩散与氧同位素退化交换作用 总被引：2，自引：0，他引：2
本文从理论上解论上解析了同位素封闭体系内的矿物氧扩散性质，火成岩从冷却为质岩从高峰变质温度冷却过程中的所发生的扩散作用会层致矿物晶体内部及晶粒间的氧同位素重新分配，两种不同的矿物氧扩散－同位素交换模式都可以用来模拟这种性质。实例研究进一步阐明了扩散对氧同位素组成的影响。 相似文献
2.
激光探针分析在氧同位素地球化学研究中的应用 总被引：6，自引：0，他引：6
简要介绍了氧同位素分析的最新方法———激光探针法的主要特点,并详细评述了激光探针分析在氧同位素地球化学研究中的应用。某些矿物内部存在氧同位素组成的变化,构成氧同位素环带。与其他化学成分环带一样,矿物氧同位素环带也可以分为生长环带（包括次生加大的环带）和扩散环带两种。变质岩中石榴石经常保存有明显的生长环带,而矽卡岩中石榴石、变质花岗质岩石中锆石和蚀变花岗岩中石英等矿物均可以记录岩石形成早期的某些氧同位素特征。由于这种差异与岩石的形成环境有关,因此通过对矿物氧同位素组成的微区分析可揭示岩石的某些成因信息。在缓慢冷却的变质岩中,磁铁矿的氧同位素环带常是扩散作用形成的,由此可以确定岩石的冷却速率。通过对脉石英的激光探针分析,可以研究流体的流动机理。变质岩的氧同位素微区分析为ｐ Ｔ ｔ ｆ轨迹研究提供了有力的武器,而氧同位素示踪可用来解决流体在变质岩形成过程中的作用问题。 相似文献
3.
矿物氧同位素模式温度计算 总被引：6，自引：1，他引：5
根据对现遥氧扩散模型的解析分析,通过模拟矿物之间的氧同位素交换轨迹进行模式温度计算,改进了常规矿物对氧同位素地质温度计方法。将模式温度计算与矿物氧－扩散封闭次上结合,建立了一个系统独立的同位素温度计算方法,因此所得到的同位素温度能够更好地反映矿物在高温岩石冷却过程中,的氧同位素交换行为;模式温度计算有如下优点：（１）考虑到了矿物之间扩散引起的同位素交换;（２）遵循质量守恒原理,更严格地适用于有限封 相似文献
4.
流体-岩石相互作用过程中氧同位素交换地球化学动力学评述 总被引：2，自引：0，他引：2
氧同位素研究对于示踪流体—岩石相互作用过程中流体的时间累积流量(或流体／岩石比)、流动方向和组成具有重要意义。基于质量平衡原理可以建立“封闭”体系和开放体系的氧同位素交换模型。“封闭”体系又可分为封闭、批式挥发和瑞利挥发体系。瑞利挥发较批式挥发造成岩石更大的^18O亏损，但在地质过程中两者差异并不显著。开放体系连续模型中氧同位素迁移的机制包括扩散称散和平流。由流体流动速率和扩散称散系数定义的Peclet数决定了上述两种机制在一定尺度上对氧同位素迁移的相对贡献。流体—岩石交换受表面动力学控制，当交换速率快于流体流动时，可认为流体和岩石达到了氧同位素分馆平衡，反之则没有达到平衡。由流体流动速率和流体—岩石反应速率常数定义的Damkoehler数决定了反应接近平衡的程度。如果采用多种矿物相监控，则矿物内部分馆可有效地区分这两种反应模型。对流体—岩石相互作用过程中氧同位素变化的地球化学动力学进行了系统评述，其原理和模型也可扩展到对其他元素的研究。 相似文献
5.
报道了大别造山带西南部湖北红安榴辉岩和罗田麻粒岩的氧同位素组成，并讨论了氧扩散作用对矿物氧同位素平衡的影响，结果得到，红安榴辉岩的全岩δ^18O值为6．4－7．3‰，罗田黄土岭麻粒岩的全岩δ^18O值为6．6－7．8‰，罗田惠兰山麻粒岩的全岩δ^18O值为3．9‰，这些榴辉岩和麻粒岩全岩的氧同位素组成保持了峰期变质条件下的平衡分馏特征，得到的氧同位素温度对于红安榴辉岩425－620度，对于罗田麻粒岩为740－945度。根据快速颗粒边界扩散模型计算的矿物对氧同位素温度不仅与大多数实测氧同位素温度一致，而且与岩石学测温结果相吻合，因此，这些岩石与东大别榴辉岩一样在形成后经历了快速冷却过程，退变质反应过程中没有外来流体加入。 相似文献
6.
矿物之间的元素和同位素平衡:地质测温和等时线定年的热力学和动力学控制 总被引：1，自引：0，他引：1
在特定的地质事件过程中,矿物等时线放射体系是否达到并且保持了平衡是变质岩Sm-Nd和Rb-Sr同位素年代学中的一个重要问题。在这个问题上矿物对O同位素测温与矿物等时线定年相似,因此两者之间可以相互制约。在岩浆岩和变质岩中,矿物中Sm-Nd、Sr和O之间的扩散速率在无水的条件下一般具有可比性,因此矿物之间O同位素的平衡状态可以用来对Sm-Nd和Rb-Sr定年的有效性进行检验。对大别-苏鲁造山带超高压变质岩的Sm-Nd和Rb-Sr等时线矿物进行O同位素测温,得到Sm-Nd等时线有时给出三叠纪年龄,有时给出非三叠纪年龄;对应的矿物O同位素分馏分别处于平衡和不平衡状态。对于引起非三叠纪等时线年龄的原因,一方面可以是由于榴辉岩相变质过程中同位素体系没有达到平衡,另一方面则可能角闪岩相退变质作用打破了平衡。等时线矿物中初始同位素比值的均一化速率主要受慢扩散矿物的影响,而矿物等时线时钟的启动主要受高母/子比值矿物控制。因此在变质作用过程中,只有当高母/子比值矿物同时具有快的放射成因同位素扩散速率,才可能得到有效的矿物等时线来用于变质年龄的测定。根据不同矿物中不同元素在扩散速率上的差异,能够定量估计大陆碰撞过程中榴辉岩相变质的持续时间。应用增量方法和离子孔隙度经验模型,不仅分别能够从理论上准确计算所有固体矿物的氧同位素分馏系数和获得不同矿物中元素的扩散参数,而且分别能够定量预测热力学平衡条件下共生矿物之间的18O富集顺序和相同条件下矿物中元素扩散速率的相对快慢。 相似文献
7.
胶南榴辉岩矿物氧同位素平衡及其Sm-Nd年代学制约 总被引：2，自引：4，他引：2
对苏鲁地体中的胶南榴辉岩进行了矿物氧同位素分析，并与同一手标本矿物的Sm-Nd内部等时线定年和Nd-Sr同位素分布进行了对比。研究表明，石榴子石与绿辉石之间的氧同位素平衡与否能够对矿物Sm-Nd同位素体系的平衡状况和内部等时线定年结果的有效性给予直接制约。合理的石榴子石＋绿辉石Sm-Nd内部等时线年龄产于两矿物之间达到并在峰变质条件下保持氧同位素平衡的样品中，而两矿物之间处于氧同位素不平衡的样品不能给出正确的Sm-Nd内部等时线年龄。同一矿物在手标本尺度出现显著的O-Nd-Sr同位素不均一性，据此对这些元素在石榴子石和绿辉石中的扩散速率顺序进行了估计，不仅得到了与实验扩散系数相吻合的结果，而且由此估计出在峰变质条件下达到矿物内部同位素均一化所需要的时间应大于10Ma。 相似文献
8.
利用增量方法对云母族矿物的氧同位素分馏进行了系统的理论计算。结果表明，不同化学成分和结构状态的云母之间存在一定的氧同位素分馏，其１８Ｏ富集顺序在热力学同位素平衡时为：多硅白云母＞钠云母＞锂云母＞白云母＝珍珠云母＞海绿石＞铁云母＞金云母＞黑云母。在４００℃以上的高温条件下，云母－水体系的氧同位素分馏与温度之间的相关性不明显，并且云母相对于水亏损１８Ｏ达１‰－２．５‰。石英－云母体系的氧同位素分馏与温度之间具有显著的负相关性，因此，能够作为灵敏的同位素地质温度计。不过，石英－黑云母对的氧同位素地质测温往往给出岩石冷却过程中的退化再平衡温度，而不是岩石形成温度。 相似文献
9.
北大别主簿源花岗岩和片麻岩矿物的 总被引：10，自引：2，他引：10
对大别造山带北部主簿源中生代花岗岩侵入体及其围岩片麻岩进行了矿物氧同位素分析，同时对同一样品进行了矿物 Rb- Sr内部等时线定年。结果表明，花岗岩和片麻岩矿物的氧同位素温度大小顺序为：角闪石 >磁铁矿 >榍石 >石英 >黑云母 >长石，遵循缓慢冷却条件下扩散控制的氧同位素交换封闭顺序，指示这些岩石没有受到后期热液蚀变的扰动。根据黑云母-长石-磷灰石-全岩内部 Rb- Sr等时线测定，花岗岩的年龄为 (118± 3) Ma，代表了岩浆侵位冷却年龄；片麻岩的年龄为 (122± 1) Ma，代表了片麻岩受大面积燕山期岩浆侵位热烘烤达到高温同位素平衡后的冷却年龄。因此，矿物之间的氧同位素平衡与否 ,能够对矿物 Rb- Sr体系封闭后平衡状态的保存性以及矿物内部等时线定年的有效性予直接制约。 相似文献
10.
地壳流体－岩石氧同位素交换反应动力学研究现状 总被引：1，自引：0，他引：1
矿物－流体体系氧同位素交换反应动力学模型主要分为５种：封闭、＂封闭＂、一般开放、流体缓冲体系以及岩石缓冲体系。交换机制主要为扩散控制和表面控制。层状辉长岩上部、下部岩系辉石往往表现出不同的交换速率和交换程度，流体的初始δ１８Ｏ值也显示出较大的不均一性。花岗岩－流体氧同位素交换反应绝大多数为开放体系不平衡类型。中深成岩基与浅成岩体在有效反应时限、流体标准化渗透率方面不同。前寒武纪条带状硅质铁建造分为低级变质地带（Ⅰ组）和高级变质地带（Ⅱ组），前者多为典型的开放体系不平衡类型，石英反应程度低；后者则接近平衡，石英反应程度高。造山带低级变质地体流体－岩石１８Ｏ交换主要是在岩石缓冲体系下进行的。流体循环与质量传输机制主要有：平流、扩散、扩散－平流复合机制。 相似文献
11.
The granulites of the Fraser Range are assumed to have formed in a carbon-rich fluid, and are generally devoid of hornblende, and lack obvious hydrous retrograde features. In these granulites, pyroxene, garnet, plagioclase and quartz are the minerals most likely to retain the oxygen isotope ratios fixed at an early stage of initial granulite metamorphism. Temperature estimates using these minerals commonly suggest that oxygen isotopic exchange ceased in the range 600 to 680°C. The peak metamorphic temperature was probably ～ 850°C as based on the stability fields of the coexisting minerals and some cation temperatures from coexisting pyroxenes in these rocks. Ilmenite may be slightly out of isotopic equilibrium with the other minerals. Thus, grains of quartz, feldspar, pyroxene and ilmenite have suffered considerable oxygen isotopic exchange during the retrogressive phase of the metamorphism, in spite of the fact that very little water was present in these granulites. The observed deviation from the peak metamorphic temperatures can be explained by essentially closed system solid-state diffusion (on at least a scale of centimetres) during slow cooling of the rocks from ~850 to 650°C, followed by more rapid cooling down to ～ 300°C. Such an explanation is not at variance with the radiometric data available for rocks from the area, which suggest that the latter phase could have involved uplift rates of ?0.5 mm/yr for a period of about 40 Ma. Wholerock δ18O values on non-quartzose mafic granulites, about 7.2%., fall within the range of basalts affected by seafloor weathering. 相似文献
12.
Experimental hydrogen isotope studies III: Diffusion of hydrogen in hydrous minerals,and stable isotope exchange in metamorphic rocks 总被引：4，自引：0，他引：4
Colin M. Graham 《Contributions to Mineralogy and Petrology》1981,76(2):216-228
Diffusion parameters for hydrogen diffusion in epidote-group minerals and micas have been measured under hydrothermal conditions, or calculated from existing experimental data, for bulk hydrogen isotope exchange experiments between hydrous minerals and water. Activation energies in the range 14 to 31 kcals/g-atom H are comparable to those derived by application of kinetic theory to experimental hydrogen isotope exchange data, and to those for oxygen diffusion in minerals under hydrothermal conditions. Diffusion of hydrogen in epidote is about four orders of magnitude faster than in muscovite, and about two orders of magnitude faster than in zoisite. Hydrogen diffusion in micas is about five orders of magnitude faster than oxygen diffusion, and hydrogen transport occurs dominantly parallel to the layers rather than parallel to the c-axis as for oxygen.Rapid hydrogen transport in minerals may proceed by hydrolysis of Si-O and Al-O bonds, followed by exchange of hydrolyzed oxygens with slower-diffusing (OH) or H2O. Water appears to be essential for stable isotope exchange between minerals in slowly cooling metamorphic rocks.Stable isotope data for regional metamorphic mineral assemblages suggests that water is usually present in small amounts during cooling of prograde regional metamorphic systems, and estimated closure temperatures for cessation of stable isotope exchange are often more comparable to those calculated from diffusion data than to likely temperatures of metamorphism.Alpine deformation of the Hercynian Monte Rose Granite (Frey et al. 1976) permitted access of water and initiated stable isotope exchange amongst coexisting minerals. The diffusional behaviour of species in relict Hercynian muscovites is consistent with available experimental diffusion data. 相似文献
13.
G. R. T. JENKIN C. M. FARROW A. E. FALLICK D. HIGGINS 《Journal of Metamorphic Geology》1994,12(3):221-235
Retrograde exchange of oxygen isotopes between minerals in igneous and metamorphic rocks by means of diffusion is explored using a finite difference computer model, which predicts both the zonation profile of δ18 O within grains, and the bulk δ18 O value of each mineral in the rock. Apparent oxygen isotope equilibrium temperatures that would be observed in these rocks are calculated from the δ18 O values of each mineral pair within the rock. In systems which cool linearly from a sufficiently high temperature or at a low enough cooling rate, such that the final oxygen isotope values are not dependent upon the initial oxygen isotope values ('slow cooling'), the apparent oxygen isotope temperature derived for a rock composed of a single mineral pair can be shown to be simply related to the Dodson closure temperatures ( T c ) for the two phases and the mode of the rock. Adding a third phase into a system which undergoes 'slow' cooling will cause the apparent temperature derived for the two minerals already present to differ from the simple relationship for a two-phase system. In some systems oxygen isotope reversals can be developed. If cooling is not 'slow', then the mineral δ18 O values resulting from cooling will be partly dependent upon the initial temperature of the system concerned. The model successfully simulates the mineral δ18 O values that are often observed in granitic rocks. Application of the model will help in assessing the validity of oxygen isotope thermometry in different geological settings, and allows quantitative prediction of the oxygen isotope fractionations that are developed in cooling closed systems. 相似文献
14.
Huaiwei Ni 《中国地球化学学报》2014,33(2):125-130
Oxygen isotope fractionation between coexisting minerals in slowly cooled rocks conveys information about their cooling history. By using the fast grain boundary （FGB） model to simulate closed-system diffusive ex- change of oxygen isotopes between coexisting minerals, I show that the apparent equilibrium temperatures （Tae） by the mineral pair with the largest isotopic fractionation （PLIF） always lies between the closure temperatures （To） of those two minerals. Therefore, when the rate of oxygen diffusion and hence Tc for the PLIF chance to be comparable （such as in the case of quartz and magnetite）, Tae will serve as a good approximation of To regardless of variation in mineral proportions. The specialty of the PLIF in constraining Tac within their Tc range can be generalized to other stable isotope systems and element partitioning. By approximating Tc with Tac and inverting Dodson＇s equation, the cooling rate of plutonic or metamorphic rocks can be inferred. 相似文献
15.
Abstract Oxygen and hydrogen isotope analyses have been made of coexisting quartz, ilmenite, muscovite, and biotite from Late Precambrian metapelitic rocks, staurolite-kyanite to K-feldspar-muscovite-sillimanite zones, from Mica Creek, British Columbia. The δ18 O and †D values of these minerals are generally uniform and do not decrease significantly with increasing metamorphic grade. This implies that there has not been significant infiltration of deep crustal, possibly magmatic, fluids into the metapelites that has been suggested for other high-grade metamorphic terranes. The uniformity of oxygen isotope compositions of the Mica Creek metapelite rocks may reflect isotopic uniformity in the sedimentary protolith rather than widespread exchange with an isotopically homogeneous metamorphic pore fluid.
Temperature estimates based upon18 O exchange thermometry for samples below the sillimanite zone are in reasonable agreement with the results of garnet-biotite Fe–Mg exchange thermometry. In the higher grade rocks, the oxygen isotope and garnet-biotite thermometry yield results which disagree by about 100°C. The highest temperatures recorded by oxygen isotope thermometry, 595°C, are at least 60°C below the minimum temperatures required by phase equilibria. These discrepancies appear to result from pervasive equilibrium retrograde exchange of oxygen isotopes between coexisting minerals. In addition, there are problems with calibration of garnet-biotite thermometry at higher temperatures. Retrograde oxygen isotope exchange may be a general characteristic of high-grade metamorphic rocks and oxygen isotope thermometry may not usually record peak metamorphic temperatures if they significantly exceed 600°C. 相似文献
Temperature estimates based upon
16.
J. Farquhar Thomas Chacko David J. Ellis 《Contributions to Mineralogy and Petrology》1996,125(2-3):213-224
Preservation of high-temperature mineral isotopic compositions is necessary for successful high-temperature isotopic thermometry.
Other requirements include large fractionations between constituent minerals, well-calibrated equilibria, carefully designed
sampling strategies and data handling techniques that quantitatively account for retrograde exchange. Here, we apply isotopic
thermometry and data handling techniques to calculate and contrast mineral-pair apparent temperature data and observed closure
temperature data (T
c-observed) (cf. Farquhar et al. 1993) for the very high temperature (>900°C), dry granulites of the Taltson Magmatic Zone of Northwestern
Canada and the Napier Complex of Enderby Land, Antarctica. The isotopic compositions of garnet grains from both terrains reflect
high temperature conditions (>950°C) and point to this mineral as an excellent candidate for isotopic thermometry. The isotopic
compositions of quartz, pyroxene, ilmenite and magnetite indicate that they equilibrated to lower temperature conditions (<900°C)
due to faster rates of oxygen diffusion in these minerals, possibly enhanced by exsolution and ductile deformation, compared
with garnet. Our temperature data for garnet and pyroxene are ≈200°C higher than is possible to explain by existing “wet”
diffusion data, but is consistent with “dry” diffusion data, suggesting that the extremely dry nature of these rocks may have
played a significant role in the preservation of high-temperature isotopic compositions. Both quartz and magnetite exhibit
subgrain features, indicative of ductile deformation. Quartz-magnetite temperatures from the Napier complex are similar to
those inferred for a late (D3) deformation and are lower than those predicted by “dry” diffusion data. We infer that the quartz-magnetite
isotopic fractionations reflect deformation-enhanced exchange that accompanied D3. Garnet in these same samples did not undergo
ductile deformation and did not exchange oxygen with coexisiting phases during cooling. This may reflect strain partitioning
between less easily deformed, low abundance garnet and more easily deformed matrix quartz and magnetite. The resistance of
garnet to ductile deformation in these rocks is a second reason why garnet is suitable for isotopic thermometry.
Received: 6 February 1996 / Accepted: 25 April 1996 相似文献
17.
Oxygen isotope study of metamorphic and granitic rocks of the Yanai district in the Ryoke belt,Japan
18O/16O ratios have been obtained for 134 whole-rocks and minerals from metamorphic and granitic rocks of the Yanai district in the Ryoke belt, Southwest Japan. The 18O/16O ratios of pelitic rocks of the marginal metamorphic zone decrease progressively with increasing metamorphic grade. In the gneiss-granite complex (zone of migmatite [1]), the most characteristic feature of the rocks is that oxygen isotopic homogenization proceeds on both local and regional scales in parallel with “granitization” or chemical homogenization. Granitic rocks of various origin are fairly uniform in isotopic composition with δ 18O of quartz of 12 to 14‰ (SMOW) and δ 18O of biotite of 7 to 9‰ and are about 3 to 4‰ enriched in 18O compared to other Cretaceous granites of non-metamorphic terranes in Japan. The high 18O/16O ratios of granitic rocks of this district were discussed in relation to the 18O-depletion in metasediments. Oxygen isotopic fractionations among coexisting minerals from various rock-types of the gneiss-granite complex indicate that these minerals were formed under near isotopic equilibrium at a temperature of about 600 to 700° C. Some abnormal fractionations of quartz-biotite pairs also were obtained for rocks which had undergone a progressive 18O-depletion or 18O-enrichment. This is due to high resistivity of quartz and contrastive susceptibility of biotite to isotopic exchange during metamorphism and “granitization”. 相似文献
18.
Oxygen isotopic compositions of silicate inclusions in IVA iron meteorites have been measured with an in situ UV laser microprobe technique. The homogeneity of oxygen isotopic compositions within and among individual mineral grains has also been examined. Oxygen isotope fractionations between coexisting mineral pairs were utilized in oxygen isotope thermometry. Our measured Δ17O values, ranging from 0.97 to 1.25‰, are characteristic of a single reservoir and fully confirm the oxygen isotopic similarity between IVA irons and L/LL chondrites. Steinbach and São João Nepomuceno, containing inclusions of two silicate minerals in mutual contact, exhibit a mass-dependent fractionation of 18O/16O between tridymite and bronzite with apparent oxygen isotopic heterogeneity. The SiO2-bearing member, Gibeon, gives homogeneous oxygen isotopic compositions without detectable fractionation of 18O/16O between tridymite and quartz. Oxygen isotope equilibrium temperatures are estimated for coexisting tridymite and bronzite in the same sample slabs or clusters in Steinbach and São João Nepomuceno. The fractionations of 18O/16O between bronzite and tridymite range from 1.6 to 2.3‰ in different sample slabs or clusters. On the basis of the closure temperature concept, cooling rates are estimated at approximately 20 to 1000°C/Myr between 800 and 1000°C, a range of temperatures not accessible to other cooling rate methods. Using the Fast Grain Boundary diffusion model, we have demonstrated that significant oxygen heterogeneity both in tridymite and bronzite is probably due to isotope exchange during cooling between minerals with various grain sizes and mineral abundances in different regions of the samples. The new estimates of cooling rate by oxygen isotope thermometry refine previous cooling curves of IVA irons and support the breakup-reassembly model for the IVA parent body. 相似文献
19.
Oxygen isotope analyses of quartz-Al2SiO5 pairs have been made for samples from the Mica Creek area, British Columbia. We have analysed quartz–kyanite nodules and quartz–kyanite and quartz–sillimanite in multiphase pelitic rocks from the staurolite–kyanite, kyanite, and sillimanite zones. Apparent temperatures calculated from oxygen isotopic fractionation range from 555 °C (staurolite–kyanite zone) to 695 °C (sillimanite zone). Temperatures from the quartz–kyanite nodules range from 630 to 675 °C. Some of the nodules show isotopic disequilibrium. Most of the results confirm predictions that bimineralic rocks will yield an estimate of peak metamorphic temperatures, when the less abundant mineral (an aluminium silicate) is the slower oxygen diffuser. Using cooling rates of 10–100 °C Ma?1 for the multiphase rocks, measured crystal sizes and modes, the Fast Grain Boundary diffusion model with ‘wet’ diffusion data (PH2O?1.0 kbar) yields predicted apparent temperatures which are generally lower than the measured apparent temperatures. The agreement is improved if slower diffusion coefficients are used. This suggests that f (H2O) during cooling was lower than that of the hydrothermal experiments and thus that there was little interaction with aqueous fluids of internal or external origin to modify the isotopic compositions. The measured apparent isotopic temperatures and apparent garnet–biotite Fe–Mg exchange temperatures show very poor agreement for the sillimanite zone samples, with the garnet–biotite Fe–Mg exchange temperatures generally higher than the oxygen isotope temperatures. Compared with the other calibrations that we tested the measured apparent temperatures using the Sharp calibration show the best agreeement with recently published P–T grids, although some variability in agreement is expected due to variable f (H2O) during cooling. 相似文献