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首页> 外文期刊>Journal of Contaminant Hydrology >Direct simulation of heterogeneous diffusion and inversion procedure applied to an out-diffusion experiment. Test case of Palmottu granite
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Direct simulation of heterogeneous diffusion and inversion procedure applied to an out-diffusion experiment. Test case of Palmottu granite

机译:直接模拟非均质扩散和反演程序应用于外扩散实验。 Palmottu花岗岩的测试案例

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An out-diffusion laboratory experiment using a non-reactive tracer was fitted using the Time Domain Diffusion (TDD) method. This rapid particle tracking method allows simulation of the heterogeneous diffusion based on pore-scale images and local values of diffusivities. The superimposed porosity and mineral 2D maps act as computation grids to condition diffusion pathways. We focused on a Palmottu granite sample, in which the connected pore space has a composite microstructure with cracks linking microporous minerals and is above the percolation threshold.rnThree main results were achieved: (ⅰ) When compared to the fitting obtained with one coefficient (best mean square residual R=1.6x 10~(-2)), diffusion is shown to be suitably characterised with two coefficients related to cracks and microporous minerals (best R=6.5 x 10~(-4)), (ⅱ) rather than imposing a local apparent diffusion coefficient D_a independent of the local porosity Φ, a best fit is obtained by applying Archie's relationship D_a=D_0xG with G=Φ~m to each pixel of the calculation grids (G is the geometry-factor, D_0 is the diffusion coefficient in free fluid, and m is Archie's exponent), and (ⅲ) the order of magnitude of the fitted diffusion coefficient or Archie's exponents (m=0 for microcracks and m= 1.82 for microporous minerals) is physically realistic.
机译:使用时域扩散(TDD)方法进行了使用非反应示踪剂的扩散实验室实验。这种快速的粒子跟踪方法允许基于孔隙尺度图像和扩散率的局部值模拟异质扩散。叠加的孔隙度和矿物2D映射充当计算网格,以调节扩散路径。我们将重点放在Palmottu花岗岩样品上,该样品的连通孔隙空间具有连接微孔矿物的裂纹的复合微结构,并且高于渗滤阈值.rn获得了三个主要结果:(ⅰ)与具有一个系数的拟合(最佳)相比均方差R = 1.6x 10〜(-2)),扩散被适当地表征为具有两个与裂纹和微孔矿物有关的系数(最佳R = 6.5 x 10〜(-4)),(ⅱ)而不是施加独立于局部孔隙率Φ的局部视在扩散系数D_a时,通过将阿奇关系D_a = D_0xG(G =Φ〜m)应用于计算网格的每个像素可获得最佳拟合(G是几何因子,D_0是在自由流体中的扩散系数,m是阿奇的指数),并且(ⅲ)拟合的扩散系数或阿奇的指数的数量级(对于微裂纹,m = 0;对于微孔矿物,m = 1.82)在物理上是现实的。

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