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部分饱和蒙脱石中的扩散与气流动力学

Diffusion and Gas Flow Dynamics in Partially Saturated Smectites.

作者信息

Owusu Jerry P, Karalis Konstantinos, Prasianakis Nikolaos I, Churakov Sergey V

机构信息

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

Institute of Geological Sciences, University of Bern, 3012 Bern, Switzerland.

出版信息

J Phys Chem C Nanomater Interfaces. 2023 Jul 17;127(29):14425-14438. doi: 10.1021/acs.jpcc.3c02264. eCollection 2023 Jul 27.

DOI:10.1021/acs.jpcc.3c02264
PMID:37529667
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10389780/
Abstract

Clays and clay rocks are considered good natural and engineered barriers for deep geological disposal of nuclear waste worldwide. Metal corrosion and organic waste degradation in underground repositories generate significant amounts of gas that should be able to migrate through the multibarrier system to avoid potential pressure buildup, which could be compromising the integrity of the barriers and host rocks. The gas is expected to accumulate in larger pores and eventually form an interconnected network. Under such conditions, the migration of gas molecules takes place both in pore water films and gas-filled macropores. Therefore, mass fluxes depend on the distribution of gas molecules between the water-rich and gas-rich phases and their mobility in both compartments. Classical molecular dynamics (MD) simulations were employed to investigate the mobilities of He, H, CO, Ar, and CH in a Na-montmorillonite mesopore as a function of the degree of saturation, as well as evaluate the hydrodynamic behavior of the pore fluid in partially saturated clays. The diffusivity of the gas molecules was determined by observing the asymptotic behavior of the mean square displacement in the gas-rich phase and at the gas-water interface. The partition coefficient and Gibbs free energy were analyzed to investigate the transfer of gas molecules between the gas-rich and water-rich phases by observing the molecular trajectories as they cross the vapor-liquid interface. The results revealed that the diffusion coefficient in the gas phase increased with increasing gas-filled pore width and converged asymptotically toward the diffusion coefficient in the bulk state. It could be shown that the diffusion coefficient of gas molecules dissolved in the water films remained constant as long as the interacting water surface was in the bulk-liquid-like phase. This behavior changes in very thin water films. It was observed that the partitioning coefficient of gas molecules at the solid-liquid interface is nearly the same as that in the bulk-liquid-like phase. Partitioning is observed to be strongly dependent on the temperature and gas molecular weights. In the second part of the study, nonequilibrium molecular dynamics (NEMD) simulations were performed to investigate the mobility of gases in pressure-driven decoupled gas-phase dynamics (DGPD) and coupled gas and water phase dynamics (CGWPD) in a partially saturated Na-montmorillonite slit mesopore. The dynamic viscosity of the gas phase was calculated from NEMD simulations and indicated that the viscosity of the gas phase was almost the same in both methods (DGPD and CGWPD). The average slip length for gas molecules at the gas-water interface was also calculated, revealing that the slip-free boundary condition assumed in continuum models is generally invalid for microfluidics and that a slip boundary condition exists at the microscale for specific surface interactions. Finally, a Bosanquet-type equation was developed to predict the diffusion coefficient and dynamic viscosity of gas as a function of the average pore width, gas mean-free path, geometric factor, and thickness of the adsorbed water film.

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5579/10389780/d850304f3da4/jp3c02264_0010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5579/10389780/d850304f3da4/jp3c02264_0010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5579/10389780/d850304f3da4/jp3c02264_0010.jpg
摘要

在全球范围内,黏土和黏土岩被视为核废料深层地质处置的良好天然及工程屏障。地下储存库中的金属腐蚀和有机废物降解会产生大量气体,这些气体应能够通过多屏障系统迁移,以避免潜在的压力积聚,因为压力积聚可能会损害屏障和围岩的完整性。预计这些气体会在较大孔隙中积聚并最终形成相互连通的网络。在这种情况下,气体分子在孔隙水膜和充满气体的大孔隙中都会发生迁移。因此,质量通量取决于气体分子在富水相和富气相间的分布以及它们在两个隔室中的迁移率。采用经典分子动力学(MD)模拟研究了钠蒙脱石中孔内He、H、CO、Ar和CH的迁移率与饱和度的关系,并评估了部分饱和黏土中孔隙流体的流体动力学行为。通过观察富气相和气 - 水界面处分子平方位移的渐近行为来确定气体分子的扩散率。通过观察分子轨迹穿过气 - 液界面时的情况,分析分配系数和吉布斯自由能,以研究气体分子在富气相和富水相之间的转移。结果表明,气相中的扩散系数随着充气孔隙宽度的增加而增大,并渐近地趋向于体相状态下的扩散系数。可以看出,只要相互作用的水表面处于类似体相液体的相中,溶解在水膜中的气体分子的扩散系数就保持不变。在非常薄的水膜中这种行为会发生变化。观察到气体分子在固 - 液界面处的分配系数与在类似体相液体的相中几乎相同。观察到分配强烈依赖于温度和气体分子量。在研究的第二部分,进行了非平衡分子动力学(NEMD)模拟,以研究部分饱和的钠蒙脱石狭缝中孔内压力驱动的解耦气相动力学(DGPD)和耦合气 - 水相动力学(CGWPD)中气体的迁移率。从NEMD模拟计算出气相的动态粘度,结果表明两种方法(DGPD和CGWPD)中气相的粘度几乎相同。还计算了气体分子在气 - 水界面处的平均滑移长度,结果表明连续介质模型中假设的无滑移边界条件通常不适用于微流体,并且在微尺度上对于特定的表面相互作用存在滑移边界条件。最后,开发了一个博赞奎特型方程,以预测气体的扩散系数和动态粘度与平均孔隙宽度、气体平均自由程、几何因子以及吸附水膜厚度的函数关系。

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本文引用的文献

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