孔隙尺寸分布的比较:以西澳大利亚页岩气地层为例

Adnan Al Hinai , Reza Rezaee , Lionel Esteban , Mehdi Labani
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引用次数: 201

摘要

对西澳大利亚北部珀斯盆地三叠系Kockatea组和二叠系Carynginia组页岩孔隙结构进行了表征。多孔介质的输运性质受相互连接的孔隙空间的拓扑结构和几何形状的调节。在同一来源的样品上,通过压汞毛细管压力(MICP)、低场核磁共振(NMR)和氮气吸附(N2)三种实验室实验进行对比,评估微观、中观和宏观孔隙度。利用高分辨率FIB/SEM图像分析进一步支持亚微米尺度下的实验孔隙结构解释。在基于MICP的中孔范围内,主要的孔喉半径约为6 nm,孔隙率约为3%。这种相对快速的实验提供了可靠的优势,在孔喉尺寸为2纳米的井屑或岩屑上。而氮气吸附法通过在相对压力下吸附的水蒸气量来确定总孔体积,可以记录2nm以下的孔径。但在制备过程中,宏观孔隙和部分细观孔隙被破坏甚至破坏。BET比表面积结果通常显示5至10 m2/g的狭窄范围。MICP和N2测量结果在孔径分类上存在不一致,主要是由于它们各自的下限和上限孔径分辨率限制。核磁共振T2弛豫时间显示的充水孔隙比MICP测试平均大30%。在再饱和实验后,由水与粘土相互作用产生的人工裂缝的证据可以解释这种孔隙度高估。从Timur-Coates核磁共振模型中提取的计算孔体孔喉比,并根据渗透率实验进行校准,表明这种孔隙几何形状直接控制渗透率,而不同页岩气地层之间和同一地层内的孔隙度和孔径分布保持相似。结合MICP、N2和NMR获得的孔隙尺寸分布似乎可以完全覆盖页岩气的孔隙尺寸范围,并克服单个方法的限制。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Comparisons of pore size distribution: A case from the Western Australian gas shale formations

Pore structure of shale samples from Triassic Kockatea and Permian Carynginia formations in the Northern Perth Basin, Western Australia is characterized. Transport properties of a porous media are regulated by the topology and geometry of inter-connected pore spaces. Comparisons of three laboratory experiments are conducted on the same source of samples to assess such micro-, meso- and macro-porosity: Mercury Injection Capillary Pressure (MICP), low field Nuclear Magnetic Resonance (NMR) and nitrogen adsorption (N2). High resolution FIB/SEM image analysis is used to further support the experimental pore structure interpretations at sub-micron scale.

A dominating pore throat radius is found to be around 6 nm within a mesopore range based on MICP, with a common porosity around 3%. This relatively fast experiment offers the advantage to be reliable on well chips or cuttings up the pore throat sizes >2 nm. However, nitrogen adsorption method is capable to record pore sizes below 2 nm through the determination of the total pore volume from the quantity of vapour adsorbed at relative pressure. But the macro-porosity and part of the meso-porosity is damaged or even destroyed during the sample preparation.

BET specific surface area results usually show a narrow range of values from 5 to 10 m2/g. Inconsistency was found in the pore size classification between MICP and N2 measurements mostly due to their individual lower- and upper-end pore size resolution limits. The water filled pores disclosed from NMR T2 relaxation time were on average 30% larger than MICP tests. Evidence of artificial cracks generated from the water interactions with clays after re-saturation experiments could explain such porosity over-estimation. The computed pore body to pore throat ratio extracted from the Timur–Coates NMR model, calibrated against gas permeability experiments, revealed that such pore geometry directly control the permeability while the porosity and pore size distribution remain similar between different shale gas formations and/or within the same formation. The combination of pore size distribution obtained from MICP, N2 and NMR seems appropriate to fully cover the range of pore size from shale gas and overcome the individual method limits.

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