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一种基于芯片实验室的方法,集成原位表征和反应传输模拟诊断,以揭示(钡,锶)硫酸盐的震荡分带现象。

A lab-on-a-chip approach integrating in-situ characterization and reactive transport modelling diagnostics to unravel (Ba,Sr)SO oscillatory zoning.

机构信息

Institute of Energy and Climate Research (IEK-6): Nuclear Waste Management and Reactor Safety, Forschungszentrum Jülich GmbH, 52425, Jülich, Germany.

Laboratory for Waste Management, Paul Scherrer Institut, 5232, Villigen PSI, Switzerland.

出版信息

Sci Rep. 2021 Dec 8;11(1):23678. doi: 10.1038/s41598-021-02840-9.

DOI:10.1038/s41598-021-02840-9
PMID:34880298
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8654837/
Abstract

The co-precipitation of sulphate minerals such as celestine and barite is widely studied because their formation is ubiquitous in natural and anthropogenic systems. Co-precipitation in porous media results in crystallization of solid solutions yielding characteristics such as oscillatory zoning that are rarely observed in bulk solution or in batch experiments. In the past, the precipitation of compositionally-zoned (Ba,Sr)SO crystals was observed post-mortem in macroscopic silica gel counter-diffusion experiments. Their formation was originally explained by the difference in the solubility products of the end-members combined with diffusion-limited transport of solutes to the mineral-fluid interface, while a later study favored the idea of kinetically controlled reactions. With recent advances combining in-operando microfluidic experiments and reactive transport modelling, it is now possible to verify hypotheses on the driving forces of transport-coupled geochemical processes. We developed a "lab on a chip" experiment that enabled the systematic study of the nucleation and growth of oscillatory-zoned (Ba,Sr)SO crystals in a microfluidic reactor. The compositions of the solid solutions were determined by in-situ Raman spectroscopy. Our investigation shows (1) that the composition of the nucleating phases can be approximated using classical nucleation theory, (2) that the oscillatory zoning is not solely controlled by the limited diffusional transport of solutes, and (3) that nucleation kinetics plays a major role in the switch between different stoichiometric compositions. The zoning phenomena is governed by the complex interplay between the diffusion of reactants and the crystallization kinetics as well as other factors, e.g. surface tension and lattice mismatch.

摘要

硫酸盐矿物(如天青石和重晶石)的共沉淀现象被广泛研究,因为它们的形成在自然和人为系统中无处不在。多孔介质中的共沉淀导致固溶体的结晶,产生特征,如很少在体相溶液或批量实验中观察到的振荡分带。过去,在宏观硅胶对扩散实验中死后观察到具有成分分带(Ba,Sr)SO 晶体的沉淀。它们的形成最初是通过端元溶解度产品的差异以及溶质扩散受限传输到矿物-流体界面来解释的,而后来的一项研究则倾向于动力学控制反应的想法。随着结合在位微流控实验和反应传输建模的最新进展,现在可以验证关于传输耦合地球化学过程驱动力的假设。我们开发了一种“芯片上实验室”实验,能够在微流反应器中系统地研究振荡分带(Ba,Sr)SO 晶体的成核和生长。通过原位拉曼光谱确定固溶体的组成。我们的研究表明:(1)成核相的组成可以使用经典成核理论近似,(2)振荡分带不仅受溶质有限扩散传输的控制,(3)成核动力学在不同化学计量组成之间的转换中起着重要作用。分带现象受反应物扩散和结晶动力学以及其他因素(如表面张力和晶格失配)之间的复杂相互作用控制。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/290fd4ce86c1/41598_2021_2840_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/b74116f7354c/41598_2021_2840_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/d55757244aed/41598_2021_2840_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/6003fcca67b3/41598_2021_2840_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/32f112c8661a/41598_2021_2840_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/814d24f4a462/41598_2021_2840_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/d38b110eeda3/41598_2021_2840_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/a0a64275d66e/41598_2021_2840_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/5f2147d00874/41598_2021_2840_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/290fd4ce86c1/41598_2021_2840_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/b74116f7354c/41598_2021_2840_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/d55757244aed/41598_2021_2840_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/6003fcca67b3/41598_2021_2840_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/32f112c8661a/41598_2021_2840_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/814d24f4a462/41598_2021_2840_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/d38b110eeda3/41598_2021_2840_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/a0a64275d66e/41598_2021_2840_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/5f2147d00874/41598_2021_2840_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3eee/8654837/290fd4ce86c1/41598_2021_2840_Fig9_HTML.jpg

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