异形结构内甲烷赋存态模拟

Molecular simulations on the occurrence states of methane in heteromorphic pores

  • 摘要: 为了研究有机质孔隙形状对甲烷赋存状态的影响,建立了与实际较为相符的碳基椭圆孔隙和带有突出与凹陷特征的异形孔隙。在特定的页岩气储层温压条件下,使用分子动力学方法模拟甲烷的赋存状态。模拟结果表明,椭圆孔隙第1吸附层密度峰值为0.565 g/cm3,小于圆形孔隙第1吸附层密度(峰值为0.620 g/cm3),椭圆孔隙第2吸附层密度峰值为0.482 g/cm3,大于圆形孔隙第2吸附层密度(峰值为0.408 g/cm3)。“突出”孔隙与“凹陷”孔隙中的突出部分均有甲烷聚集,由于壁面原子的势能影响,甲烷聚集后出现空缺,空缺的存在导致第1吸附层断开,断开程度受特征点处曲率半径大小影响,另外“突出”孔隙中的断开程度比“凹陷”孔隙中的明显。同时发现,“突出”孔隙中甲烷的平均密度大于“凹陷”孔隙中甲烷的平均密度。孔隙中游离气的存在特征受孔隙形状的影响。“突出”孔隙中,随着特征点处的曲率半径减小,游离气逐渐减小直至几乎消失。“凹陷”孔隙中,随着特征点处的曲率半径减小,凹陷部分的甲烷第2吸附层逐渐向无凹陷部分移动,最终导致两部分的第2吸附层重合,孔隙中的游离气几乎消失。研究结果表明,孔隙形状的改变会对甲烷在孔隙中的平均密度、分布规律产生明确影响,甲烷的赋存状态与孔隙形状密切相关。

     

    Abstract: In order to investigate the effect of the shapes of organic matter pores on occurrence states of methane, the carbon-based elliptical pore and the heteromorphic pores with the characteristics of protrusion and depression were established more consistently with the fact. The occurrence states of methane were simulated by using the molecular dynamics method under the temperature and pressure of gas reservoir. The simulation results show that the density of the first adsorption layer in elliptical pore (peak 0.565 g/cm3) is smaller than that of the first adsorption layer in circular pore (peak 0.620 g/cm3), and the density of the second adsorption layer in elliptical pore (peak 0.482 g/cm3) is larger than that of the second adsorption layer in circular pore (peak 0.408 g/cm3). Methane accumulated in the protrudent parts of“protrusion”pores and“depression”pores, and there is a vacancy near methane accumulation because of the atoms potential of wall. The first adsorption layer breaks which caused by the vacancy. The degree of breakage is influenced by the curvature radius of the feature point, and the degrees of breakage in“protrusion”pores are more obvious than those in“depression” pores. At the same time, it is found that the mean density of“protrusion” pores is higher than that of“depression”pores. The characteristics of free gas in the pores are influenced by the shapes of the pores. In the“protrusion”pores, with the curvature radius of feature point decrease, the free gas gradually decreases until almost disappears. In the“depression” pores, with the curvature radius of feature point decrease, second adsorption layer of methane in depression part gradually move towards non depression part, and finally, the second adsorption layers of two parts overlap, and the free gas in the pores almost disappears. The results show that the mean density and distribution pattern of methane is definitely affected by the pore shape that the occurrence states of methane are closely related to the pore shapes.

     

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