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Fluid distribution effects on P-wave velocity of CO2/brine saturated rocks: a comparison study and implications for CO2 storage monitoring using seismic method

机译:流体分布对CO2 /盐水饱和岩石的P波速度的影响:使用地震方法对CO2储存监测的比较研究和影响

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The evaluation of fluid saturation using P-wave velocity is affected by the fluid distribution at mesoscale significantly. Here we present the experimental results of two tests for measuring P-wave velocity under ultrasonic frequencies in two different rocks (one sandstone and one tuff, respectively) during CO2 displacing brine. Both tests were performed under a high injection pressure of 10 MPa in order to control CO2 in a supercritical state. The two rock samples display differences in rock heterogeneity. The sandstone sample shows obvious layered structures with high and low porosity layers, whereas the tuff sample shows a near homogeneous structure. During the dynamic fluid displacements tests, we used X-ray CT technique to image rock interior frequently and then calculated average CO2 saturation near the local wave propagation path. The results show very different saturation-velocity relationships for the two tests. The sandstone sample gives a relationship that is close to Gassmann-Hill limit, whereas the tuff sample gives a relationship located near the Gassmann-Wood limit. Meanwhile, X-ray CT images show the distribution of CO2 in the sandstone sample is more heterogeneous and larger fluid patches are developed in it during CO2 drainage. In contrast, the tuff sample shows the development of very small and dispersed CO2 patches and relatively well mixing state of CO2 and brine in the rock. We then use the random patchy saturation model to interpret the results theoretically. The results indicate that the characteristic patch size is in an order of tens of millimeters in the experiment using sandstone sample, whereas it is smaller than 0.1 mm in the experiment using tuff sample. Whether the scale of the strong-contrast heterogeneity created by patchy CO2 saturation is significant to wave velocity is determined by the ratio of patch size and fluid diffusion length (AIL ratio), which is a function of wave frequency and hydraulic diffusion coefficient of the rock. If the scale of the heterogeneity is larger than the fluid diffusion length at a wave frequency, the strain field created by wave propagation cannot be relaxed during a half period and the media shows the stiffening effect-a higher velocity at macroscale. These suggest that one should pay attenuation to the effect of fluid distribution and degree of phase mixing when evaluating fluid saturation from P-wave velocity using seismic methods, if the reservoir develops significant large-scale heterogeneity. Furthermore, the velocity becomes insensitive to saturation changes when CO2 saturation becomes higher than approximately 0.2, if its changes follow the Gassmann-Wood relationship (with small AIL ratio at lower frequencies). In contrast, the velocity remains changing widi CO2 saturation at higher CO2 saturation if the changes follow the Gassmann-Hill relationship (with large AIL ratio at higher frequencies). The changes suggest the selection of wave frequency is critical to validly monitor the saturation changes at higher CO2 saturations.
机译:使用P波速度的流体饱和度的评估受Mesoscale的流体分布显着影响。在这里,我们在CO 2位移盐水期间,介绍了两种不同岩石(分别)在两种不同岩石(一个砂岩和一个凝灰岩)中的超声频率下的P波速度的试验结果。这两个测试都在10MPa的高注射压力下进行,以便在超临界状态下控制CO 2。两个岩石样本显示岩石异质性的差异。砂岩样品显示具有高孔隙层和低孔隙层的明显分层结构,而凝灰套样品显示出近均匀的结构。在动态流体位移测试期间,我们经常使用X射线CT技术对图像岩石内部,然后计算局部波传播路径附近的平均CO2饱和度。结果显示了两个测试的饱和速度关系非常不同。砂岩样品提供了靠近Gassmann-Hill限制的关系,而Tuff样本则提供了位于Gassmann-Wood限制附近的关系。同时,X射线CT图像显示砂岩样品中的CO2的分布是更异质的,在CO 2引流期间在其上开发出较大的流体贴片。相比之下,凝灰剂样品显示出非常小和分散的CO 2贴片的显影和岩石中的CO 2和盐水的相对良好的混合状态。然后我们使用随机拼接饱和模型理论上解释结果。结果表明,使用砂岩样品在实验中的特征贴片尺寸为数十毫米,而使用Tuff样品,实验中的实验小于0.1mm。是否通过斑块CO2饱和产生的强对比度异质性的规模是显着的波速度的是通过贴片尺寸和流体扩散长度(AIL比率)的比率来确定,这是岩石的波频和液压扩散系数的函数。如果异质性的比例大于波频以流体扩散长度,则在半周期内不能松弛波传播产生的应变场,并且介质在宏观上表示加强效果 - 更高的速度。这些表明,如果储层产生显着的大规模异质性,则应在评估来自P波速度的流体饱和时的流体分布和相相混合程度的效果。此外,如果二氧化碳饱和度高于约0.2,则速度变化变化变化,如果其变化遵循Gassmann-Wood关系(在较低频率下的比率小)。相反,如果变化遵循Gassmann-Hill关系(在较高频率下的大比率大),则速度仍然在较​​高的CO2饱和度下仍然在更高的CO2饱和度下变化Widi CO2饱和度。该更改表明波频的选择对于有效地监视较高CO2饱和度的饱和度变化至关重要。

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