Speaker
Description
With an ever-increasing global warming scenario, geological sequestration stands as an effective mean to trap gases such as carbon dioxide (CO
Our analogue experiment is based on refractive index matching of the fluid (a solution of Triton X-100, water and zinc chloride) to the solid grains (spherical PMMA beads, which renders the 3D porous medium transparent. The density contrast between the heavier and lighter (miscible) liquid phases comes from the amount of ZnCl2 added, while the heavier fluid also contains a dye (at a small concentration) to allow tracking the interface evolution and fingering structures. Varying the density of the heavier fluid and the PMMA bead size allows controlling the Rayleigh (Ra) and Darcy (Da) numbers. Measurements are performed in quasi-two-dimensional conditions. The data consists of images recorded at a regular time interval and post-processed using MATLAB. Darcy scale numerical simulations of the experimental configuration are performed using the software COMSOL Multiphysics. The experimental and numerical results are compared in terms of the mixing length, finger velocity and finger number density. We observe that the presence of the granular porous medium strongly impacts the gravitational instability dynamics (as compared to the simulated dynamics), and this all the more as the characteristic number Ra√Da is larger. For Ra√Da>1 the simulation results largely under-predicts the experimental data. More importantly, this under-prediction doesn’t cancel out entirely when the Darcy regime is valid (Ra√Da<0.1), i.e., when the typical scale of convection fingers is larger than the pore size. This finding mays suggest that the coupling between gravity-actuated Stokes flow and solute transport cannot be simply upscaled to the Darcy scale using coupled Darcy’s law and a dispersive solute transport equation.
References
[1] Bachu, S. (2008). CO2 storage in geological media: Role, means, status and barriers to deployment. Progress in energy and combustion science, 34(2), 254-273.
[2] Raza, A., Rezaee, R., Bing, C. H., Gholami, R., Hamid, M. A., & Nagarajan, R. (2016). Carbon dioxide storage in subsurface geologic medium: A review on capillary trapping mechanism. Egyptian Journal of Petroleum, 25(3), 367-373.
[3] Kumar, S., Foroozesh, J., Edlmann, K., Rezk, M. G., & Lim, C. Y. (2020). A comprehensive review of value-added CO2 sequestration in subsurface saline aquifers. Journal of Natural Gas Science and Engineering, 103437.
[4] Gilfillan, S. M., Lollar, B. S., Holland, G., Blagburn, D., Stevens, S., Schoell, M., ... & Ballentine, C. J. (2009). Solubility trapping in formation water as dominant CO 2 sink in natural gas fields. Nature, 458(7238), 614-618.
[5] Baines, S. J., & Worden, R. H. (2004). Geological storage of carbon dioxide. Geological Society, London, Special Publications, 233(1), 1-6.
[6] Emami-Meybodi, H., Hassanzadeh, H., Green, C. P., & Ennis-King, J. (2015). Convective dissolution of CO2 in saline aquifers: Progress in modeling and experiments. International Journal of Greenhouse Gas Control, 40, 238-266.
[7] Vreme, A., Nadal, F., Pouligny, B., Jeandet, P., Liger-Belair, G., & Meunier, P. (2016). Gravitational instability due to the dissolution of carbon dioxide in a Hele-Shaw cell. Physical Review Fluids, 1(6), 064301.
[8] Pau, G. S., Bell, J. B., Pruess, K., Almgren, A. S., Lijewski, M. J., & Zhang, K. (2010). High-resolution simulation and characterization of density-driven flow in CO2 storage in saline aquifers. Advances in Water Resources, 33(4), 443-455.
[9] Nadal, F., Meunier, P., Pouligny, B., & Laurichesse, E. (2013). Stationary plume induced by carbon dioxide dissolution. Journal of Fluid Mechanics, 719, 203-229.
[10] Meunier, P., & Nadal, F. (2018). From a steady plume to periodic puffs during confined carbon dioxide dissolution. Journal of Fluid Mechanics, 855, 1-27.
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