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Quantifying the Occurrence of Shale Oil in Nanoconfined Kerogen Matrices through Integrated NMR Relaxation Theory and Molecular Dynamics Simulations

干酪根 油页岩 吸附 分子动力学 纳米孔 放松(心理学) 化学物理 烷烃 化学 分子 扩散 材料科学 分子扩散 碳氢化合物 癸烷 基质(化学分析) 矿物学 页岩油 热力学 类金刚石 致密油
作者
Yansong Gu,Liqiang Yang,Xinmin Ge,Qun Zhang,Liangwei Xu,Chao Fang,Peiwen Xiao,Bing Liu
出处
期刊:Langmuir [American Chemical Society]
卷期号:41 (45): 30594-30608 被引量:2
标识
DOI:10.1021/acs.langmuir.5c04334
摘要

Low-field nuclear magnetic resonance (NMR) is a powerful technique for characterizing fluid behavior in shale oil reservoirs. However, the abundant nanopores in shale and the limitations of experimental echo time hinder its further application in characterizing oil occurrence. This study integrates the ratio of longitudinal to transverse relaxation times (T1/T2) with molecular dynamics simulations to determine the distributions of dissolved, adsorbed, and free n-decane in kerogen nanoslits and further develops quantitative models to characterize the occurrence characteristics of n-decane in these confined systems. The results indicate that alkane molecules in the same state exhibit identical T1/T2 values, with the T1/T2 values of dissolved, adsorbed, and free molecules being 25.27, 18.61, and 14.86, respectively. For each occurrence state, both the self-diffusion coefficient of n-decane and its interaction energy with the kerogen nanoslit walls exhibit distinct linear correlations with T1/T2. Furthermore, three mathematical models are developed to quantify the relationships between T1/T2 and the slit width, the adsorption layer thickness (H), and the free-to-adsorbed mass ratio (mf/ma). When T1/T2 ranges from 75.21 to 53.25, mf/ma = 0, indicating the absence of a free state. This state corresponds to slit widths of 1–3 nm, within which H varies linearly with T1/T2. As T1/T2 decreases further from 53.25 to 1.00, mf/ma increases exponentially while H stabilizes at ∼2.86 nm, suggesting three-state coexistence within 3–50 nm slits. Free-state dominance occurs when T1/T2 approaches 1, corresponding to a slit width of approximately 50 nm. Additionally, with increasing kerogen maturity, the kerogen matrix exhibits reduced solubility but enhanced adsorption capacity for n-decane. For kerogen types I-A, II-D, and III-A, T1/T2 shows exponential correlations with both slit width and mf/ma, indicating free-state dominance at slit widths of 45, 50, and 58 nm, respectively. This work is expected to provide novel insights into shale reservoir evaluation and enhanced oil recovery.
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