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Pore-scale simulation of carbonate dissolution in micro-CT images

机译:微型CT图像中碳酸盐溶解的孔隙度模拟

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We present a particle-based method to simulate carbonate dissolution at the pore scale directly on the voxels of three-dimensional micro-CT images. The flow field is computed on the images by solving the incompressible Navier-Stokes equations. Rock-fluid interaction is modeled using a three-step approach: solute advection, diffusion, and reaction. Advection is simulated with a semianalytical pore-scale streamline tracing algorithm, diffusion by random walk is superimposed, while the reaction rate is defined by the flux of particles through the pore-solid interface. We derive a relationship between the local particle flux and the independently measured batch calcite dissolution rate. We validate our method against a dynamic imaging experiment where a Ketton oolite is imaged during CO2-saturated brine injection at reservoir conditions. The image-calculated increases in porosity and permeability are predicted accurately, and the spatial distribution of the dissolution front is correctly replicated. The experiments and simulations are performed at a high flow rate, in the uniform dissolution regime-Pe 1 and PeDa 1thus extending the reaction throughout the sample. Transport is advection dominated, and dissolution is limited to regions with significant inflow of solute. We show that the sample-averaged reaction rate is 1 order of magnitude lower than that measured in batch reactors. This decrease is the result of restrictions imposed on the flux of solute to the solid surface by the heterogeneous flow field, at the millimeter scale.
机译:我们提出了一种基于粒子的方法,可以直接在三维微CT图像的体素上模拟碳酸盐在孔尺度上的溶解。通过求解不可压缩的Navier-Stokes方程在图像上计算流场。岩石与流体的相互作用采用三步法建模:溶质对流,扩散和反应。用半解析孔尺度流线追踪算法模拟对流,叠加通过随机游走的扩散,而反应速率由通过孔-固界面的颗粒通量定义。我们推导了局部颗粒通量和独立测量的批次方解石溶解速率之间的关系。我们通过动态成像实验验证了我们的方法,该实验通过在储层条件下注入CO2饱和盐水的过程中对Ketton卵石成像。可以精确预测通过图像计算得出的孔隙度和渗透率的增加,并且可以正确复制溶蚀锋面的空间分布。实验和模拟是在高流速下进行的,在均匀的溶出度-Pe 1和PeDa 1中进行,从而将反应扩展到整个样品中。运输以对流为主,溶解仅限于溶质大量流入的区域。我们表明,样品平均反应速率比间歇反应器中测量的平均速率低1个数量级。这种减少是由于异质流场限制了溶质通向固体表面的通量(毫米级)的结果。

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