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Effect of elastic instability on mobilization of capillary entrapments

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Shakeri,  Pegah
Group Geometry of Fluid Interfaces, Department of Dynamics of Complex Fluids, Max Planck Institute for Dynamics and Self-Organization, Max Planck Society;

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Jung,  Michael
Group Geometry of Fluid Interfaces, Department of Dynamics of Complex Fluids, Max Planck Institute for Dynamics and Self-Organization, Max Planck Society;

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Seemann,  Ralf
Group Geometry of Fluid Interfaces, Department of Dynamics of Complex Fluids, Max Planck Institute for Dynamics and Self-Organization, Max Planck Society;

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Citation

Shakeri, P., Jung, M., & Seemann, R. (2021). Effect of elastic instability on mobilization of capillary entrapments. Physics of Fluids, 33: 113102. doi:10.1063/5.0071556.


Cite as: https://hdl.handle.net/21.11116/0000-0009-800F-6
Abstract
The flow of viscoelastic polymer solutions and their use as displacing agents in porous media are important for industrial applications, such
as enhanced oil recovery and soil remediation. The complexity of flow and high elasticity of conventionally used viscoelastic polymer
solutions can lead to purely elastic instability in porous media. In this study, we investigate the impact of this instability on displacing
capillary entrapments at low Reynolds numbers using a microfluidic approach. Our unique design consists of a single-capillary entrapment
connected to two symmetric serpentine channels. This design excludes the effect of viscous forces and enables a direct focus on displacement
processes driven solely by elastic forces. After the onset of purely elastic instability, an unstable base flow is observed in the serpentine channels.
We discuss that the pressure fluctuations caused by this unstable flow create an instantaneous non-equilibrium state between the two
ends of the capillary entrapment. This provides the driving pressure to overcome the capillary threshold pressure and eventually displace the
entrapped oil. In our geometry, we observe that the displacement coincides with the emergence of a fully developed elastic turbulent state.