Geological carbon sequestration
A promising technique for mitigation of the rising level of atmospheric CO
2 and global warming is carbon capture and storage (CCS). This relies on subsurface storage of CO
2, mainly in deep saline aquifers (but also in unminable coal seams or depleted oil and gas reservoirs). Following the injection of CO
2 (in supercritical form) it undergoes several processes that control the rates and volume that could be safely stored, and the associated risk (e.g. of leakage or induced seismicity). However, these processes and their interplay with the medium microstructure and reactive transport mechanisms remain poorly understood.
One of the mechanisms that keeps the CO
2 in place is dissolution trapping: the supercritical CO
2 (scCO
2) dissolves by diffusion into the brine to increase its density beyond that of the original brine, sinking deeper which makes it less prone to leakage. This process if often accelerated by a convective (gravitationally-driven) instability in the forms of fingers of denser CO2-rich brine sinking downwards, which in turn accelerates the rate of dissolution of further scCO
2 into the brine at the top.
Emmanuel Luther's PhD thesis addresses the onset of this instability and its impact on later stages via linear stability analyses (LSA) and reservoir simulations. Specifically, we are interested in the impact of the medium structure, in particular permeability variations in the form of layering which is prevalent in geological formations used for CCS. Our analysis shows that even a thin perturbation in permeability (
Int. J. Greenh. Gas Control. 2021) and its inclination [in preparation] could greatly impact the onset of convective instability.
Another desired trapping mechanisms which also constitutes a fascinating open scientific problem is mixing-induced precipitation (MIP) of minerals, mainly carbonates. Particularly, the effects of small-scale heterogeneity (e.g. pore size variations), and the consequent non-uniform flow and precipitation at the km-scale of interest to CCS remain elusive. In a coming project, we will combine microfluidic experiments with pore network modelling to expose the underlying physics of MIP from the single pore to the sample level, including the effect of dimensionality (2D to 3D) and of the high pressures of real CCS conditions. We will then use reservoir modelling to upscale these insights to the field scale.