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石墨狭缝吸附页岩气的分子模拟
引用本文:何映颉,杨 洋,张廷山,伍坤宇. 石墨狭缝吸附页岩气的分子模拟[J]. 岩性油气藏, 2016, 28(6): 88-94. DOI: 10.3969/j.issn.1673-8926.2016.06.012
作者姓名:何映颉  杨 洋  张廷山  伍坤宇
作者单位:1.油气藏地质与开发工程国家重点实验室·西南石油大学,成都610500; 2.西南石油大学地球科学与技术学院,成都610500; 3.中国石油青海油田分公司勘探开发研究院,甘肃敦煌736202
基金项目:国家自然科学基金青年基金项目“甲烷在页岩气储层微纳米孔隙系统中运移的动力学机理研究”(编号:41302123)及博士学科点专项科研基金项目“页岩微观储集空间发育特征及其对页岩气赋存富集的影响机理”(编号:20125121130001)联合资助
摘    要:为了深入了解页岩储层中有机质层状孔隙对甲烷的微观吸附机理,利用分子模拟软件构建了石墨狭缝模型来表征有机质层状孔隙,并运用巨正则蒙特卡罗、分子力学及分子动力学等方法模拟了扬子板块早古生代页岩储层在埋深为2~4 km 的条件下,石墨狭缝对甲烷的吸附性能。结果表明:石墨狭缝对甲烷的吸附是物理吸附;随温度和压力的增加,其吸附量呈现出先急剧增加后缓慢增加再减小的趋势;当页岩气藏埋深为2~4 km 时,页岩储层中有机质层状孔隙对甲烷的吸附量缓慢增加,并且在埋深为4 km 时达到最大,因此4 km 为页岩气最优埋深;甲烷沿石墨狭缝壁法线方向出现明显的吸附分层现象,其相对密度呈对称分布的趋势,而且随埋深的增加而有所减小;甲烷的自扩散系数随埋深的增加而增大,与吸附热及吸附量的变化原因一致。

关 键 词:岩石  渗透率  气体  滑脱效应  Klinkenberg效应  Knudsen数  
收稿时间:2016-06-13

Molecular simulation of shale gas adsorption in graphite slit-pores
He Yingjie,Yang Yang,Zhang Tingshan,Wu Kunyu. Molecular simulation of shale gas adsorption in graphite slit-pores[J]. Northwest Oil & Gas Exploration, 2016, 28(6): 88-94. DOI: 10.3969/j.issn.1673-8926.2016.06.012
Authors:He Yingjie  Yang Yang  Zhang Tingshan  Wu Kunyu
Affiliation:(1. State Key Laboratory of Oil & Gas Reservoir Geology and Exploitation, Southwest Petroleum University, Chengdu 610500, China;2. School of Resources and Environment, Southwest Petroleum University, Chengdu 610500, China; 3. Research Institute of Exploration and Development, PetroChina Qinghai Oilfield Company, Dunhuang 736202, Gansu, China)
Abstract:In order to understand the methane adsorption mechanism in organic matter pores in shale, graphite slit-pores were established to characterize the organic matter pores by using molecular simulation software, the grand canonical Monte Carlo method, molecular mechanics and molecular dynamics were used to simulate methane adsorption in graphite slit-pores at the common shale burial depth of 2-4 km in Yangtze Plate. The results show that the adsorption was physical. With the increasing of temperature and pressure, the adsorption capacity in graphite slit-pores increased dramatically first, then increased slowly, and decreased at last, and the maximum adsorption capacity appeared at the buried depth of 2-4 km (4 km is the best buried depth for shale gas). The relative density of methane along the normal direction of the graphite slit-pore wall shows a trend of symmetric distribution, which reflects apparent adsorption stratification, and it reduced with the increase of buried depth. The self-diffusion coefficient of methane increased with the increase of buried depth, which is consistent with the changes of adsorption heat and adsorption capacity.
Keywords:rock   permeability   gas   slippage effect   Klinkenberg effect   Knudsen number  
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