Fracture Intensity Impacts on Reaction Front Propagation and Mineral Weathering in Three‐Dimensional Fractured Media

Author:

Andrews E. M.123ORCID,Hyman J. D.3ORCID,Sweeney M. R.3ORCID,Karra S.4ORCID,Moulton J. D.5,Navarre‐Sitchler A.2ORCID

Affiliation:

1. Deparment of Earth, Environmental and Resource Sciences University of Texas at El Paso El Paso TX USA

2. Hydrologic Science and Engineering Colorado School of Mines Golden CO USA

3. Computational Earth Science Group (EES‐16) Earth and Environmental Sciences Division Los Alamos National Laboratory Los Alamos NM USA

4. Environmental Molecular Sciences Laboratory Pacific Northwest National Laboratory Richland WA USA

5. Applied Mathematics and Plasma Physics (T‐5) Theoretical Division Los Alamos National Laboratory Los Alamos NM USA

Abstract

AbstractStudying reaction front propagation in heterogeneous natural settings is challenging, but numerical simulations can provide insight into the varying spatial and temporal scales of reaction front propagation. Here, the impact of increasing fracture intensity on mineral dissolution rates, and the extent of reaction front propagation is investigated using reactive transport simulations in upscaled discrete fracture network domains with varied fracture intensity. Domain‐averaged dissolution rates vary less than 0.5 log units regardless of the fracture intensity, but the spatial distribution of reactions is controlled by the location and number of dead‐end fractures and the number of connected flowpaths through the domain. Higher fracture intensities lead to more weathering in the domain because of more available mineral for water‐rock interactions. We find that reaction fronts propagate through the primary flowpaths in the first 10,000 years of the simulation for a 10‐m length domain, then propagate into secondary flowpaths and dead‐end fractures between 10,000 and 100,000 years, and finally into the matrix over timescales of hundreds of thousands of years. The domain‐averaged reaction rates decrease through time corresponding to a transition from dissolution in advection‐dominated, fast‐flowing pathways, to dissolution in transport‐limited zones of disconnected fractures and matrix. Matrix dissolution, or dissolution under transport‐limited conditions, is the dominant process at late times in these simulations. The results of these simulations recreate the observed paradox found in nature where highly fractured hillslopes tend to be more weathered but have slower weathering rates, while hillslopes with fewer fractures, are less weathered but have higher dissolution rates.

Funder

Division of Earth Sciences

Los Alamos National Laboratory

Publisher

American Geophysical Union (AGU)

Subject

Water Science and Technology

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