Published June 18, 2006
| Version v1
Conference paper
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Linking Experimental Capillary Pressure-Saturation Data with Lattice Boltzmann Simulations.
Authors/Creators
- 1. University of California, Riverside and GEBJ Salinity Lab
- 2. nstitute of Environment & Resources, Technical University of Denmark, DK-2800 Kongens Lyngby, Denmark
- 3. Department of Geosciences, Oregon State University, Corvallis, OR 97331, USA
Description
Recent advances in observational and computational techniques have facilitated the
study of fluid dynamics and interfacial geometry in porous media. Within some
experimental limitations, computed tomography X-ray (CMT) and magnetic resonance
imaging (MRI) are now able to accurately map the 3D structure of porous geometries.
Computational advances largely concern Lattice Boltzmann (LB) method that has been
shown to be useful in simulating microscale flow in porous media. With some
phenomenological or thermodynamic extensions, the LB method is also able to deal with
microscale interfacial phenomena in single or multiphase systems.
The goal of this presentation is to provide insight into what is needed to make a
link between 3D experimental observations of interfacial geometry and LB simulations.
The experimental data consist of CMT observations several Sotrol-water displacements
inside a glass bead system with a resolution of 17 microns. Also available are
capillary pressure-saturation curves between 0 and 1kPa. The LB model is that of
Shan-Chen as modified by Martys and Chen (1996). We present the most parsimonious
way to calibrate the surface tension and contact angle in the model, define space,
pressure and time scaling. We will also identify potential problems relating to
pore-size and digitization effects that are present in the simulations, but not in
the original observations. The analyses are partly performed on idealized systems
and finally applied to large scale (107 voxel) simulations of the real physical
systems. Observations are simulations are compared in terms of pressure-saturation
curves, and where possible, in terms of fluid distribution and interfacial curvatures.
Notes
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