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Experimental study of capillary trapping on the pore scale for various sandstone cores

机译:各种砂岩核心毛细管诱捕毛细管的实验研究

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Entrapment of the non-wetting phase in porous media has been observed in a variety of fields such as petroleum engineering, geological storage of carbon dioxide, and remediation of ground water. We investigated gas trapping in porous media from a microscopic point of view. Highresolution, three-dimensional images of pore structure and trapped gas bubbles in Berea sandstones were obtained using a micro-focused X-ray CT scanner. We used vertical and horizontal Berea sandstone cores, 8 mm in diameter and 15 mm long. Based on the three-dimensional image analysis, the statistical distribution of the trapped gas volume was estimated. Trapped bubbles have a pore-network scale size and distribute over several pores. In the case of the vertical core, the porosity fluctuates along the flow direction due to the layered structure. The residual gas saturation also fluctuates with porosity along the flow direction. The higher gas saturation in porous layers at the end of gas injection results in a higher trapped gas saturation compared to dense layers. On the other hand, in dense layers the gas saturation at the end of gas injection is almost the same as the residual gas saturation. Therefore, most of the gas injected into the dense layers would be trapped. In the case of horizontal core, the gas saturation at the irreducible water condition is lower than that for the vertical core, because the injected gas selectively passes through the more permeable layers. However, the residual gas saturation is 29.2% for the horizontal core, which is comparable with that for the vertical core (30.9%). Finally, the effect of capillary number on stability of trapped gas bubbles has been estimated. Trapped gas bubbles are stable against the increased flow rate up to a capillary number of 1.0 ×10~(-5).
机译:在多孔介质中捕获在多孔介质中的非润湿相,例如石油工程,二氧化碳地质储存和地下水的修复。我们从微观的角度调查了多孔介质的气体捕获。使用微聚焦的X射线CT扫描仪获得孔隙结构的高级度,孔隙结构的三维图像和Berea Sandstones的捕获气泡。我们使用垂直和水平的耳砂砂岩,直径为8毫米,长15毫米。基于三维图像分析,估计捕获的气体体积的统计分布。被困的气泡具有孔隙网络尺度尺寸并在几个孔隙上分布。在垂直芯的情况下,由于层状结构,孔隙率沿着流动方向波动。残留的气体饱和度也沿着流动方向与孔隙率波动。气体注射末端的多孔层中的气体饱和度较高,导致与致密层相比更高的捕获气体饱和度。另一方面,在致密层中,气体喷射末端的气体饱和与残余气体饱和度几乎相同。因此,喷射到密集层中的大部分气体将被捕获。在水平芯的情况下,不可缩续的水条件下的气体饱和度低于垂直芯的气体饱和度,因为注入的气体选择性地穿过更渗透层。然而,水平芯的残留气体饱和度为29.2%,与垂直芯(30.9%)相当。最后,估计了毛细数字对捕获气泡稳定性的影响。捕获的气泡与增加的流速增加到1.0×10〜(-5)的毛细管。

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