花岗岩和伟晶岩中富水熔体包裹体作为超临界状态的“冷冻”样品揭示了在非平衡条件下产生的极端元素富集

IF 0.5 Q4 MINERALOGY
R. Thomas, P. Davidson, A. Rericha, D. Voznyak
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引用次数: 6

摘要

在这一贡献中,我们表明在富水熔体结晶过程中,这些矿物形成熔体的样品以富水熔体包裹体的形式被捕获,主要保存在石英中。水的体积浓度和温度是系统的决定参数,因为从他们的分析可以得出,这些熔体包裹体在温度和水浓度的坐标上描绘了伪二元溶解度曲线。此外,使用简化坐标(H2O/ h2crit vs. T/Tcrit),所研究的伟晶岩的大多数熔体包裹体在标准化和简化的溶剂曲线中绘制得很好。这种均匀溶液曲线的存在和形成是在接近平衡条件下结晶过程的一种表现。然而,熔体包裹体的许多微量元素和一些主要元素被捕获在溶剂峰附近[H2O/ h2crit从0.5到1.5和T/Tcrit > 0.95],呈现出不寻常的分布,具有非常明确的高斯和/或洛伦兹曲线,其特征是定义了面积、宽度、偏移量和高度。这已在许多从伟晶岩中获得的自然例子中得到证明。只有偏移值代表接近平衡状态和相应的元素浓度,这相当于区域克拉克数(克拉克数或克拉克是一种化学元素的相对丰度,通常在地壳中)。我们将这些分布解释为这个关键区域的一些特殊化学性质:主要是极高的扩散速率,低动态粘度和极低的表面张力。在临界点附近,我们有空间和时间相关的非平衡和平衡过程紧密相连。此外,我们可以证明高斯分布和洛伦兹分布是特定元素分布的第一次近似,因为在临界点,某些元素的富集达到了这样的程度,以至于高斯和/或洛伦兹曲线退化成一条垂直线(渐近于浓度轴),这是由超临界熔体-水体系中某种物质的最大溶解度决定的。以Ehrenfriedersdorf熔体包裹体中Be的最高浓度为71490 ppm为例。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Water-Rich Melt Inclusion as "Frozen" Samples of the Supercritical State in Granites and Pegmatites Reveal Extreme Element Enrichment Resulting Under Non-Equilibrium Conditions
In this contribution, we show that in miarolitic pegmatites during the crystallization of water-rich melts, samples of these mineral-forming melts were trapped in the form of water-rich melt inclusions, preserved primarily in quartz. The bulk concentration of water and the temperature are the system-determining parameters since from their analysis it follows that these melt inclusions depict pseudo-binary solvus curves in the coordinates of temperature and water concentration. Furthermore, using reduced coordinates (H2O/H2Ocrit vs. T/Tcrit) most melt inclusions of the studied pegmatites plot very well in a standardized and reduced solvus curve. The existence and formation of such uniform solvus curves is an expression of crystallization processes under nearly equilibrium conditions. However, many trace and some principal elements of the melt inclusions trapped near the solvus crest [H2O/H2Ocrit from 0.5 to 1.5 and T/Tcrit > 0.95] show unusual distributions, with very well-defined Gaussian and/or Lorentzian curves, characterized by defined area, width, offset, and height. This has been shown in many natural examples obtained from pegmatites. Only the offset values represent near-equilibrium conditions and corresponding element concentrations, which are equivalent to the regional Clarke number (Clarke number or Clark is the relative abundance of a chemical element, typically in the Earth's crust). We interpret these distributions as explanation for some extraordinary-chemical properties in this critical region: principally extremely high diffusion rates, low dynamic viscosity and extremely low surface tension. Near the critical point, we have both space and time-related non-equilibrium and equilibrium processes close together. Furthermore, we can show that the Gaussian and Lorentzian distribution are first approximations of the specific element distribution because at the critical point the enrichment of some elements reaches such an extent that the Gaussian and/or Lorentzian curves degenerate into a vertical line (are asymptotic to the concentration axis), which is determined by the maximum solubility of a species in the supercritical melt-water system. The highest concentration of Be, as an example, was observed in Ehrenfriedersdorf melt inclusions: 71490 ppm Be.
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来源期刊
CiteScore
0.70
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