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首页> 外文期刊>Geochimica et Cosmochimica Acta: Journal of the Geochemical Society and the Meteoritical Society >Theoretical calculation of oxygen isotope fractionation factors in carbonate systems
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Theoretical calculation of oxygen isotope fractionation factors in carbonate systems

机译:碳酸盐体系中氧同位素分馏因子的理论计算

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Using established methods of statistical mechanical calculation and a recent compilation of vibrational frequency data, we have computed oxygen isotope reduced partition function ratios (beta values) for a large number of carbonate minerals. The oxygen isotope beta values of carbonates are inversely correlated to both the mass and radius of the cation bonded to the carbonate anion but neither correlation is good enough to be used as a precise and accurate predictor of beta values. There is an approximately 0.6% relative increase in the beta values of aragonite per 10 kbar increase in pressure. These estimates of the pressure effect on beta values are broadly similar to those deduced previously for calcite using the methods of mineral physics. In comparing the beta values of our study with those derived recently from first-principles lattice dynamics calculations, we find near-perfect agreement for calcite and witherite (<0.3% deviation), reasonable agreement for dolomite (<0.9% deviation) and somewhat poorer agreement for aragonite and magnesite (1.5-2% deviation). In the system for which we have the most robust constraints, CO2-calcite, there is excellent agreement between our calculations and experimental data over a broad range of temperatures (0-900 degrees C). Similarly, there is good to excellent correspondence between calculation and experiment for most other low to moderate atomic mass carbonate minerals (aragonite to strontianite). The agreement is not as good for high atomic mass carbonates (witherite, cerussite, otavite). In the case of witherite and cerussite, the discrepancy may be due, in part, to our calculation methodology, which does not account for the effect of cation mass on the magnitude of vibrational frequency shifts associated with heavy isotope substitution. However, the calculations also reveal an incompatibility between the high- and low-temperature experimental datasets for witherite and cerussite. Specifically, the shapes of fractionation factor versus 1/T-2 curves in the calcite-witherite and calcite-cerussite systems do not conform to the robust constraints on the basic shape of these curves provided by theory. This suggests that either the high- or low-temperature datasets for both minerals is in error. Dolomite-calcite fractionation factors derived from our calculations fall within the wide range of fractionations for this system given by previous experimental and natural sample studies. However, our compilation of available low-temperature (25-80 degrees C) experimental data reveal an unusual temperature dependence of fractionations in this system; namely, the data indicate an increase in the magnitude of fractionations between dolomite (or proto-dolomite) and calcite with increasing temperature. Such a trend is incompatible with theory, which stipulates that fractionations between carbonate minerals must decrease monotonically with increasing temperature. We propose that the anomalous temperature dependence seen in the low-temperature experimental data reflect changes in the crystallinity and degree of cation ordering of the dolomite phase over this temperature interval and the effect these changes have on the vibrational frequencies of dolomite. Similar effects may be present in natural systems at low-temperature and must be considered in applying experimental or theoretical fractionation data to these systems. In nearly all cases, carbonate mineral-calcite fractionation factors given by the present calculations are in as good or better agreement with experimental data tha are fractionations derived from semi-empirical bond strength methods. (C) 2008 Elsevier Ltd. All rights reserved.
机译:使用统计机械计算的既定方法和振动频率数据的最新汇编,我们已经计算了许多碳酸盐矿物的氧同位素还原的分配函数比(β值)。碳酸盐的氧同位素β值与与碳酸根阴离子键合的阳离子的质量和半径均成反比,但两者之间的相关性都不足以用作β值的精确预测。每增加10 kbar压力,文石的β值相对增加约0.6%。这些对β值的压力影响的估算值与先前使用矿物物理学方法对方解石得出的估算值大致相似。通过将我们的研究的β值与最近从第一性原理晶格动力学计算得出的值进行比较,我们发现方解石和堇青石的一致性接近完美(偏差<0.3%),白云石的合理一致性(偏差<0.9%),并且较差文石和菱镁矿的一致性(偏差1.5-2%)。在我们具有最严格的约束条件的系统(方解石二氧化碳)中,我们的计算结果与实验数据在宽广的温度范围(0-900摄氏度)之间有着极好的一致性。同样,对于大多数其他低到中等原子质量的碳酸盐矿物(文石到锶锶矿),在计算和实验之间也有很好的对应关系。对于高原子质量的碳酸盐(堇青石,陶粒,陶土),该协议不那么理想。如果是铜铁矿和铜铁矿,则差异可能部分归因于我们的计算方法,该计算方法未考虑到阳离子质量对与重同位素取代相关的振动频移幅度的影响。但是,计算结果还显示了高温和低温实验数据集中有关堇青石和陶粒的不相容性。具体而言,方解石-钙铁矿和方解石-铈铁矿体系中的分馏因子与1 / T-2曲线的形状不符合理论上对这些曲线的基本形状的严格约束。这表明这两种矿物的高温或低温数据集都是错误的。从我们的计算中得出的白云石-方解石分馏因子属于先前实验和自然样品研究给出的该系统分馏范围之内。但是,我们对可用的低温(25-80摄氏度)实验数据的汇编揭示了该系统中馏分的不同寻常的温度依赖性。也就是说,数据表明白云石(或原始白云石)和方解石之间的分馏幅度随温度升高而增加。这种趋势与理论不符,后者规定碳酸盐矿物之间的分馏必须随温度升高而单调减少。我们提出,低温实验数据中看到的反常温度依赖性反映了在该温度区间内白云石相的结晶度和阳离子有序度的变化,以及这些变化对白云石振动频率的影响。在低温下的自然系统中可能会出现类似的影响,在将实验或理论分馏数据应用于这些系统时必须考虑这些影响。在几乎所有情况下,由本计算得出的碳酸盐矿物-方解石分馏因子与实验数据完全相同或更好,这是从半经验结合强度方法得出的分馏结果。 (C)2008 Elsevier Ltd.保留所有权利。

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