Initial conditions or emergence: What determines dissolution patterns in rough fractures?

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Abstract

Dissolution of fractured rocks is often accompanied by the formation of highly localized flow paths. While the fluid flow follows existing fractures in the rock, these fissures do not, in general, open uniformly. Simulations and laboratory experiments have shown that distinct channels or "wormholes" develop within the fracture, from which a single highly localized flow path eventually emerges. The aim of the present work is to investigate how these emerging flow paths are influenced by the initial aperture field. We have simulated the dissolution of a single fracture starting from a spatially correlated aperture distribution. Our results indicate a surprising insensitivity of the evolving dissolution patterns and flow rates to the amplitude and correlation length characterizing the imposed aperture field. We connect the similarity in outcomes to the self-organization of the flow into a small number of wormholes, with the spacing determined by the length of the longest wormholes. We have also investigated the effect of a localized region of increased aperture on the developing dissolution patterns. A competition was observed between the tendency of the high-permeability region to develop the dominant wormhole and the tendency of wormholes to spontaneously nucleate throughout the rest of the fracture. We consider the consequences of these results for the modeling of dissolution in fractured and porous rocks. Key Points Fracture dissolution patterns are insensitive to the initial aperture distribution Wormhole competition leads to patterns where the wormhole spacing is comparable to the length Localized regions of high permeability (vugs) can be overwhelmed by spontaneous wormhole formation.

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Upadhyay, V. K., Szymczak, P., & Ladd, A. J. C. (2015). Initial conditions or emergence: What determines dissolution patterns in rough fractures? Journal of Geophysical Research: Solid Earth, 120(9), 6102–6121. https://doi.org/10.1002/2015JB012233

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