Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
5765933 | Journal of Contaminant Hydrology | 2017 | 10 Pages |
â¢Transport transitions from non-Fickian to Fickian with increasing fracture scaleâ¢The fitted CTRW parameters are scale-insensitive for given fracture roughness.â¢The degree of non-Fickian transport is proportional to 3D fracture roughness.
Understanding transport in rough fractures from non-Fickian to Fickian regimes and the prediction of non-Fickian transport is critical for the development of new transport theories and many practical applications. Through computational experiments that fall within the macrodispersion regime, we first simulated and analyzed solute transport through synthetic rough fractures with stationary geometrical properties (i.e., fracture roughness Ïb/ãbã and correlation length λ, where b refers to aperture with its standard deviation Ïb and arithmetic mean ãbã) across increasing fracture longitudinal transport domain length L, with L/λ ranging from 2.5 to 50. The results were used to determine how solute transport behavior evolves with increasing scale in the longitudinal direction. Moreover, a set of correlated fractures with aperture fields following normal and log-normal distributions was created to further identify and quantify the dependence of non-Fickian transport on roughness. We found that although persistent intermittent velocity structures were present, the breakthrough curves (BTCs) and residence time distributions showed diminishing early arrival and tailing, features of non-Fickian transport, with increasing longitudinal L/λ, ultimately converging to a Fickian transport regime given Ïb/ãbã remained constant. Inverse analysis of the experimental BTCs with the advection-dispersion equation (ADE) model showed that the dispersion coefficient (D) was non-trivially scale-dependent. Simulation results for rough fractures with varying Ïb/ãbã and L/λ indicated that the ratio of fluid velocity to transport velocity fitted to the ADE model depends on Ïb/ãbã and L/λ. The continuous time random walk (CTRW) performed much better across all transport scales, and resulted in scale-independent fitted parameters, i.e., β in the memory function. The fitted β is proportional to Ïb/ãbãbut is insensitive to L/λ. Therefore, bulk longitudinal solute transport across the pre-asymptotic and asymptotic regimes can be estimated based on the CTRW model parameterized by measurable fracture physical properties.