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Steady flows driven by sources of random strength in heterogeneous aquifers with application to partially penetrating wells

机译:非均质含水层中随机强度源驱动的稳定流动及其在部分渗透井中的应用

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Average steady source flow in heterogeneous porous formations is modelled by regarding the hydraulic conductivity K(x) as a stationary random space function (RSF). As a consequence, the flow variables become RSFs as well, and we are interested into calculating their moments. This problem has been intensively studied in the case of a Neumann type boundary condition at the source. However, there are many applications (such as well-type flows) for which the required boundary condition is that of Dirichlet. In order to fulfill such a requirement the strength of the source must be proportional to K(x), and therefore the source itself results a RSF. To solve flows driven by sources whose strength is spatially variable, we have used a perturbation procedure similar to that developed by Indel-man and Abramovich (Water Resour Res 30:3385-3393, 1994) to analyze flows generated by sources of deterministic strength. Due to the linearity of the mathematical problem, we have focused on the explicit derivation of the mean head distribution G_d(x) generated by a unit pulse. Such a distribution represents the fundamental solution to the average flow equations, and it is termed as mean Green function. The function G_d(x) is derived here at the second order of approximation in the variance σ~2 of the fluctuation ε(x) = 1 -K(x)/K_A (where K_A is the mean value of K(x)), for arbitrary correlation function p(x), and any dimensionality d of the flow domain. We represent G_d(x) as product between the homogeneous Green function G_d~(0){x) valid in a domain with constant K_A, and a distortion term = 1 +σ~2ψd(x) which modifies G_d~(0)(x) to account for the medium heterogeneity. In the case of isotropic formations ψd(x) is expressed via one quadrature. This quadrature can be analytically calculated after adopting specific (e.g.. exponential and Gaussian) shape for p(x). These general results are subsequently used to investigate flow toward a partially-penetrating well in a semi-infinite domain. Indeed, we construct a σ~2-order approximation to the mean as well as variance of the head by replacing the well with a singular segment. It is shown how the well-length combined with the medium heterogeneity affects the head distribution. We have introduced the concept of equivalent conductivity K~(dq)(r,z). The main result is the relationship J~(eq)(r,z)/K_A = 1 -σ~2ψ~(w)(r,z) where the characteristic function ψ~(w)(r,z) adjusts the homogeneous conductivity K_A to account for the impact of the heterogeneity. In this way, a procedure can be developed to identify the aquifer hydraulic properties by means of field-scale head measurements. Finally, in the case of a fully penetrating well we have expressed the equivalent conductivity in analytical form, and we have shown that K~(efu)≤ K~(eq)(r) ≤ K_A (being K(efu)the effective conductivity for mean uniform flow), in agreement with the numerical simulations of Firmani et al. (Water Resour Res 42:W03422, 2006).
机译:通过将水力传导率K(x)视为静态随机空间函数(RSF),可以模拟非均质多孔地层中的平均稳定油源流。因此,流量变量也将成为RSF,我们对计算它们的力矩很感兴趣。在源头为Neumann型边界条件的情况下,已经对该问题进行了深入研究。但是,在许多应用程序(例如井流)中,所需边界条件是Dirichlet的边界条件。为了满足这样的要求,源的强度必须与K(x)成正比,因此源本身会产生RSF。为了解决由强度在空间上可变的源驱动的流量,我们使用了类似于Indelman和Abramovich(Water Resour Res 30:3385-3393,1994)开发的扰动程序来分析确定强度源产生的流量。由于数学问题的线性性,我们集中于显式推导单位脉冲产生的平均水头分布G_d(x)。这样的分布代表了平均流量方程的基本解,被称为平均格林函数。在此,函数G_d(x)在波动ε(x)= 1 -K(x)/ K_A的方差σ〜2中以二阶近似求出(其中K_A是K(x)的平均值)对于任意相关函数p(x)和流域的任何维数d。我们将G_d(x)表示为在常数K_A的域中有效的齐次格林函数G_d〜(0){x)与修改G_d〜(0)(的失真项= 1 +σ〜2ψd(x)之​​间的乘积x)考虑到介质的异质性。在各向同性地层的情况下,ψd(x)通过一个正交表示。可以对p(x)采用特定的形状(例如指数和高斯),然后通过解析计算得出该正交。这些一般结果随后用于研究流向半无限域中的部分渗透井的流量。实际上,我们通过用奇异段替换井来构造σ〜2阶逼近平均值和头部的方差。它显示了井长与中等非均质性相结合如何影响水头分布。我们介绍了等效电导率K〜(dq)(r,z)的概念。主要结果是关系J〜(eq)(r,z)/ K_A = 1-σ〜2ψ〜​​(w)(r,z),其中特征函数ψ〜(w)(r,z)调整齐次电导率K_A可解决异质性的影响。通过这种方式,可以开发出一种通过现场水头测量来识别含水层水力特性的程序。最后,在完全渗透的情况下,我们以分析形式表示了等效电导率,并表明K〜(efu)≤K〜(eq)(r)≤K_A(即K(efu)有效电导率平均流量),与Firmani等人的数值模拟相一致。 (Water Resour Res 42:W03422,2006)。

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