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Impact of fracture development on the effective permeability of porous rocks as determined by 2‐D discrete fracture growth modeling
Author(s) -
Paluszny A.,
Matthai S. K.
Publication year - 2010
Publication title -
journal of geophysical research: solid earth
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/2008jb006236
Subject(s) - mechanics , materials science , coalescence (physics) , fracture (geology) , geometry , mathematics , physics , composite material , astrobiology
Fracture networks exert a strong influence on fluid flow in the subsurface. We present a 2‐D linear elastic finite element model that generates fracture patterns in incremental iterative steps. A subcritical failure criterion is applied to simulate quasi‐static multiple crack propagation. We study their impact on fluid flow as a function of fracture density. Fractures are represented by closed polygons. Geomechanical apertures are a by‐product of growth and depend on the current stress state. Fracture arrest, closure, and coalescence are handled by a geometric kernel. Traction and cohesion along fracture walls are not taken into account. All patterns are generated assuming plane strain and applying displacement tensile boundary conditions. We assume randomly distributed flaw positions with a uniform probability distribution and Gaussian‐distributed flaw lengths. A piecewise fracture permeability is derived from the parallel plate law. We measure the effective permeability, k eff , and fracture‐matrix flux ratio, q f / q m across the percolation threshold. Before the percolation threshold we observe an increase in k eff of up to two orders of magnitude. Models with fixed apertures overpredict k eff by up to six orders of magnitude, as they disregard variations in the aperture distribution due to fracture interaction. After percolation our model predicts steady linear increase in effective permeability. The q f / q m ratio better captures the initial increase in hydraulic conductivity of the system as opposed to the k eff measurements. Results corroborate that fracture percolation and stress‐dependent aperture distribution due to mechanical interactions control the evolution of the k eff of the system. Results depend on the number of initial flaws used for fracture set growth.

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