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首页> 外文期刊>Doklady Earth Sciences >Possible Role of Thermal Concentration Convection during the Fractionation of Components in Basic Intrusions
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Possible Role of Thermal Concentration Convection during the Fractionation of Components in Basic Intrusions

机译:热集中对流在基础侵入体组分分离过程中的可能作用

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Concentration convection is among the factors responsible for the separation of components during the fractionation of basic melts in magma chambers. However, this factor has been disregarded in the known formulations of dynamic problems of this kind. It is likely that this situation is related to the fact that, in such formulations of the problem, attention has been focused on the volume effects of gravity phase separation. The local separation of components at the crystallization boundary is usually considered in approximation, which is used to estimate the effective coefficient of distribution k_(eff) between solid and liquid phases. The complexity of its implementation lies in the fact that it includes an unknown variable δ_C, i.e., the thickness of the diffuse boundary layer. We note that the experimental verification of theory in salt systems related to the dependence of k_(eff) on the rate of ingot consolidation, intensity of mixing, and angle of the container inclination was carried out without analyzing the factor mentioned above. We note that this factor must be taken into consideration in the analysis of the conditions of the separation of components in crystal cells in estimations of the ratio of the compositions of melted inclusions and volume liquid phase. Usually, δ_C is estimated from the solution of the problem of free convection at a stationary vertical wall. At present, we have a local automodel and a more complete solution of such a problem, in which the dependence of melt density on the local concentration of components and density jump and the phase interface are taken into account. For petrogenetic application, the use of the most complete approximation requires an additional analysis, which is given in this paper. Let us consider such a problem with a simple binary system Fe_2SiO_4 + Fe_3O_4 as an example.
机译:浓缩对流是在岩浆室内基本熔体分馏过程中导致组分分离的因素之一。但是,这种因素在这种动态问题的已知公式中已被忽略。这种情况很可能与以下事实有关:在这种问题的表述中,注意力已集中在重力相分离的体积效应上。通常近似地考虑在结晶边界处的组分的局部分离,该分离用于估计固相和液相之间的有效分布系数k_(eff)。其实现的复杂性在于它包括未知变量δ_C,即扩散边界层的厚度。我们注意到,盐体系中与k_(eff)对铸锭固结速率,混合强度和容器倾斜角度的依赖性有关的理论的实验验证是在没有分析上述因素的情况下进行的。我们注意到,在估计熔融夹杂物的组成与液相的组成之比时,在分析晶胞中组分的分离条件时必须考虑该因素。通常,δ_C是根据固定垂直壁处自由对流问题的解决方案估算的。目前,我们有一个局部自动模型和一个更完整的解决方案,其中考虑了熔体密度对组分局部浓度和密度跃变以及相界面的依赖性。对于成岩应用,使用最完整的近似值需要进行额外的分析,本文对此进行了分析。让我们以简单的二元系统Fe_2SiO_4 + Fe_3O_4为例来考虑这样的问题。

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