February 2017

Journal

Flow Regimes During Immiscible Displacement

By:
Armstrong, Ryan; Mcclure, James; Berrill, Mark A; Rucker, Maja; Schlüter, S; Berg, Steffen
Journal Name:
Petrophysics
Page Number:
10-18
Volume:
58
Issue Number:
1
Publication Date:
February 2017

Abstract

Fractional À ow of immiscible phases occurs at the pore scale where grain surfaces and phases interfaces obstruct phase mobility. However, the larger scale behavior is described by a saturation-dependent phenomenological relationship called relative permeability. As a consequence, pore-scale parameters, such as phase topology and/ or geometry, and details of the À ow regime cannot be directly related to Darcy-scale À ow parameters. It is well understood that relative permeability is not a unique relationship of wetting-phase saturation and rather depends on the experimental conditions at which it is measured. Herein we use fast X-ray microcomputed tomography to image pore-scale phase arrangements during fractional À ow and then forward simulate the À ow regimes using the lattice-Boltzmann method to better understand the underlying pore-scale À ow regimes and their inÀ uence on Darcy-scale parameters. We ¿ nd that relative permeability is highly dependent on capillary number and that the Corey model ¿ ts the observed trends. At the pore scale, while phase topologies are continuously changing on the scale of individual pores, the Euler characteristic of the nonwetting phase (NWP) averaged over a suf¿ ciently large ¿ eld of view can describe the bulk topological characteristics; the Euler characteristic decreases with increasing capillary number resulting in an increase in relative permeability. Lastly, we quantify the fraction of NWP that À ows through disconnected ganglion dynamics and demonstrate that this can be a signi¿ cant fraction of the NWP À ux for intermediate wetting-phase saturation. Rate dependencies occur in our homogenous sample (without capillary end effect) and the underlying cause is attributed to ganglion À ow that can signi¿ cantly inÀ uence phase topology during the fractional À ow of immiscible phases.


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