We investigate the stability of radial viscous fingering (VF) in miscible fluids. We show that the instability is determined by an interplay between advection and diffusion during the initial stages… Click to show full abstract
We investigate the stability of radial viscous fingering (VF) in miscible fluids. We show that the instability is determined by an interplay between advection and diffusion during the initial stages of flow. Using linear stability analysis and nonlinear simulations, we demonstrate that this competition is a function of the radius $r_{0}$ of the circular region initially occupied by the less-viscous fluid in the porous medium. For each $r_{0}$, we further determine the stability in terms of Péclet number ($Pe$) and log-mobility ratio ($M$). The $Pe{-}M$ parameter space is divided into stable and unstable zones: the boundary between the two zones is well approximated by $M_{c}=\unicode[STIX]{x1D6FC}(r_{0})Pe_{c}^{-0.55}$. In the unstable zone, the instability is reduced with an increase in $r_{0}$. Thus, a natural control measure for miscible radial VF in terms of $r_{0}$ is established. Finally, the results are validated by performing experiments that provide good qualitative agreement with our numerical study. Implications for observations in oil recovery and other fingering instabilities are discussed.
               
Click one of the above tabs to view related content.