汞侵入密实粘土的 X 射线显微层析:洞察宏观孔隙的几何形状

Shengyang YuanNAVIER UMR 8205, Xianfeng LiuNAVIER UMR 8205, Yongxin WangNAVIER UMR 8205, Pierre DelageNAVIER UMR 8205, Patrick Aimedieu, Olivier Buzzi
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引用次数: 0

摘要

润湿塌陷行为和渗透性等土壤特性与土壤微观结构密切相关。迄今为止,包括汞渗入孔隙模拟(MIP)在内的多种技术可用于表征土壤的微观结构,但所有技术都有其自身的局限性。在本研究中,通过 X 射线显微断层摄影术(X-$\mu$CT)研究了通过 MIP 试验渗入试样孔隙网络并被夹带在其中的汞的特征,以便深入了解宏观孔隙的几何形状和可能的墨水瓶几何形状。对压实的马里兰粘土选择了两种含水量和密度条件。对 MIP 后微结构中夹带的汞的分布和几何特征进行了描述,并重建了孔径分布。结果表明,在本文研究的两种条件下,大孔隙在试样中均匀分布,且大部分呈非球形,长宽比(给定段上最大厚度与最小厚度之比)小于 3。由于试验中使用的试样实验方案和墨水瓶几何形状的影响,MIP 和 X-$\mu$CT 得到的大孔的主要入口孔径不同。在 X-$\mu$CT 中,只有高纵横比的大孔体才能成像,这是由于在减压和随后制备 X-$\mu$CT 样品的过程中汞被挤出所致。在空隙率较低的样品中,由于长宽比更明显,主要入口孔径的差异更为显著。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
X-Ray microtomography of mercury intruded compacted clay: An insight into the geometry of macropores
Soil properties, such as wetting collapse behavior and permeability, are strongly correlated to the soil microstructure. To date, several techniques including mercury intrusion porosimetry (MIP), can be used to characterize the microstructure of soil, but all techniques have their own limitations. In this study, the features of mercury that penetrated and has been entrapped in the pore network of the specimens through MIP testing were investigated by X-Ray microtomography (X-$\mu$CT), in order to give an insight into the geometry of macropores and possible ink-bottle geometry. Two conditions of water content and density were selected for the compacted Maryland clay. The distribution and geometry features of mercury entrapped in the microstructure after MIP were characterized and pore size distributions were also reconstructed. The results suggest that, for the two conditions studied in this paper, macropores were evenly distributed within the specimens, and most of them with a non-spherical shape, and with aspect ratio (ratio between the maximum and minimum thickness along a given segment) smaller than three. Different dominant entrance pore size of macropore was obtained from MIP and X-$\mu$CT, due to the specific experimental protocol used in tests and the effect of ink-bottle geometry. Only the large pore bodies with high aspect ratio were imaged in X-$\mu$CT, due to the extrusion of mercury during the process of depressurization and subsequent sample preparation for X- $\mu$CT. But entire pore space was accessible in MIP. The difference in dominant entrance pore size was more significant for specimens with lower void ratio due to a more pronounced aspect ratio.
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