首页> 外国专利> Determining anisotropic diffusivity in a volume affected by microseismic activity using real volumes rather than laboratory tests as laboratory results do not scale up correctly

Determining anisotropic diffusivity in a volume affected by microseismic activity using real volumes rather than laboratory tests as laboratory results do not scale up correctly

机译:使用实际体积而非实验室测试来确定受微震活动影响的体积中的各向异性扩散率,因为实验室结果无法正确放大

摘要

A number of data sets are determined, each set representing a wavefront and including coordinates of the point of appearance and a time of first appearance at the point. A matrix is calculated by second derivation by space of a function representing the minimum appearance time of the microseismic waves as a function of the data sets. The matrix is inverted and the diffusivity tensor deduced : A front of a first appearance of microseismic waves propagating in the volume is provoked by a pressure increase in the volume caused by a source and causing the object of the measurements bearing on its location and time of appearance. The relation between the second derivation matrix and the diffusivity is D=H(- 1)/2pi , where D is the diffusivity tensor, H is the matrix obtained by second derivation of the function representing the minimum time of appearance and H(-1) represents the inverted matrix H. The volume is modelled by a mesh of cells and each set of data corresponds to a cell and includes the point of appearance corresponding to the minimum appearance time from among the measured microseismic waves which are found in the cell. The matrix is regular or non- structured (tetrahedric or stratigraphic). A function representing the minimum appearance time is calculated on the mesh by interpolating the appearance time values in the data sets and the second derivation matrix is obtained by second order spatial derivation of this function. An independent claim is made for a method of determining permeability in a volume affected by microseismic activity, giving a front of first appearance of the microseismic wave propagating in the volume, caused by an increase in pressure in the volume from a source. The diffusivity is calculated using the method above and the anisotropic permeability tensor is calculated from the anisotropic diffusivity tensor thus obtained.
机译:确定许多数据集,每个数据集代表波前并包括出现点的坐标和该点的首次出现时间。通过对空间进行二次推导来计算矩阵,该函数表示作为数据集的函数的微地震波的最小出现时间。矩阵倒置并推导扩散张量:在体积中传播的微震波的首次出现的前部是由源引起的体积压力增加引起的,并且导致测量对象取决于其位置和时间。出现。二阶导数矩阵与扩散率之间的关系为D = H(>-1)/ 2pi,其中D为扩散率张量,H为通过二次求出表示最小出现时间的函数得到的矩阵,H(> -1)表示倒置矩阵H。该体积由一个单元网格建模,每组数据对应一个单元,并且包括与在测量的微震波中发现的最小出现时间相对应的出现点。细胞。矩阵是规则的或非结构化的(四面体或地层)。通过对数据集中的出现时间值进行插值,可以在网格上计算表示最小出现时间的函数,并通过对该函数进行二阶空间推导来获得第二个导数矩阵。对确定受微地震活动影响的体积中的渗透率的方法提出了独立的权利要求,该方法给出了由于来自源的体积中的压力增加而引起的在体积中传播的微地震波的首次出现的前部。使用上述方法计算扩散率,并从由此获得的各向异性扩散率张量计算出各向异性渗透率张量。

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