东营凹陷页岩油赋存特征分子动力学模拟
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张世明(1975—),男,湖北随州人,教授级高级工程师,博士,从事油田开发理论、复杂介质油藏渗流机理及油藏数值模拟技术研究。E-mail:zhangshm855.slyt@sinopec.com。

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国家科技重大专项“低渗-致密油藏高效提高采收率新技术”(2017ZX05009-004),中国石化科研项目“济阳坳陷基质型页岩油流动机理研究”(P20058-1-2)和“东营凹陷页岩油开发优化设计技术研究”(P21060-2)。


Molecular dynamics simulation of shale oil occurrence in Dongying Depression
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    摘要:

    页岩储层储集空间主要为纳米尺度孔隙,页岩油在纳米尺度孔隙中的赋存状态对其流动规律会产生重要影响。利用核磁共振冻融技术得到了东营凹陷页岩孔隙结构的全尺寸孔径分布及纳米尺度孔隙的主频孔隙直径,基于东营凹陷牛斜55井的井流物组成,采用分子动力学模拟方法建立东营凹陷典型纳米尺度孔隙模型,开展原油在有机质纳米尺度孔隙内赋存状态研究。研究结果表明:①东营凹陷页岩储层纳米尺度孔隙的主频孔隙直径为15nm;②有机质纳米尺度孔隙内的原油密度从孔隙壁面到孔隙中央逐渐降低;③页岩油分子会在有机质纳米尺度孔隙的壁面处形成“类固体”层,其密度约为孔隙中央游离态原油密度的1.1~3.15倍;④页岩油分子在有机质纳米尺度孔隙内发生四层吸附,第1吸附层的厚度最大,计算得到东营凹陷页岩油吸附态比例为19.8%。

    Abstract:

    The storage space of shale reservoirs is mainly composed of nanoscale pores,in which the shale oil occurrence can have important influence on its flow law. The full-scale pore size distribution of shale pore structure and the main-frequency pore diameter of nanoscale pores in Dongying Depression were obtained by the nuclear magnetic resonance freezethaw(NMRF)technology. With the well effluent composition of Well NX55 in Dongying Depression,the molecular dynamics simulation was used to establish a typical nanoscale pore model of Dongying Depression,with which the occurrence of shale oil in nanoscale pores of organic matter was studied. The study results show as follow:①The main-frequency pore diameter of nanoscale pores in shale reservoirs of Dongying Depression is 15 nm;②The density of crude oil in the organic nanoscale pores gradually decreases from surface to center;③The shale oil molecules can form a“quasi-solid”layer on the walls of organic nanoscale pores,and its density is about 1.1-3.15 times that of the free crude oil in the center of the pores;④The shale oil molecules are adsorbed in four layers in organic nanoscale pores. The thickness of the first layer is the largest,and the calculated proportion of absorbed shale oil in Dongying Depression is 19.8%.

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张世明.东营凹陷页岩油赋存特征分子动力学模拟[J].油气地质与采收率,2021,28(5):74~80

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  • 在线发布日期: 2021-12-20
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