Abstract:Geological carbon storage has the potential to reduce anthropogenic carbon dioxide emissions, if large volumes can be injected and securely retained. Storage capacity is limited by regional pressure buildup in the subsurface. However, natural CO2 reservoirs in the United States are commonly underpressured, suggesting that natural processes reduce the pressure buildup over time and increase storage security. To identify these processes, we studied Bravo Dome natural CO2 reservoir (New Mexico, USA), where the ga… Show more
“…In deep geological formations the layer may not be strictly horizontal; for example, in carbon sequestration the saline aquifers are generally inclined at an angle to the horizontal [18][19][20][21].…”
We investigate the flow structure and dynamics of moderate-Rayleigh-number (
R
a
) thermal convection in a two-dimensional inclined porous layer. High-resolution numerical simulations confirm the emergence of
O
(
1
)
aspect-ratio large-scale convective rolls, with one ‘natural’ roll rotating in the counterclockwise direction and one ‘antinatural’ roll rotating in the clockwise direction. As the inclination angle
ϕ
is increased, the background mean shear flow intensifies the natural-roll motion, while suppressing the antinatural-roll motion. Our numerical simulations also reveal—for the first time in single-species porous medium convection—the existence of spatially-localized convective states at large
ϕ
, which we suggest are enabled by subcritical instability of the base state at sufficiently large inclination angles. To better understand the physics of inclined porous medium convection at different
ϕ
, we numerically compute steady convective solutions using Newton iteration and then perform secondary stability analysis of these nonlinear states using Floquet theory. Our analysis indicates that the inclination of the porous layer stabilizes the boundary layers of the natural roll, but intensifies the boundary-layer instability of the antinatural roll. These results facilitate physical understanding of the large-scale cellular flows observed in the numerical simulations at different values of
ϕ
.
“…In deep geological formations the layer may not be strictly horizontal; for example, in carbon sequestration the saline aquifers are generally inclined at an angle to the horizontal [18][19][20][21].…”
We investigate the flow structure and dynamics of moderate-Rayleigh-number (
R
a
) thermal convection in a two-dimensional inclined porous layer. High-resolution numerical simulations confirm the emergence of
O
(
1
)
aspect-ratio large-scale convective rolls, with one ‘natural’ roll rotating in the counterclockwise direction and one ‘antinatural’ roll rotating in the clockwise direction. As the inclination angle
ϕ
is increased, the background mean shear flow intensifies the natural-roll motion, while suppressing the antinatural-roll motion. Our numerical simulations also reveal—for the first time in single-species porous medium convection—the existence of spatially-localized convective states at large
ϕ
, which we suggest are enabled by subcritical instability of the base state at sufficiently large inclination angles. To better understand the physics of inclined porous medium convection at different
ϕ
, we numerically compute steady convective solutions using Newton iteration and then perform secondary stability analysis of these nonlinear states using Floquet theory. Our analysis indicates that the inclination of the porous layer stabilizes the boundary layers of the natural roll, but intensifies the boundary-layer instability of the antinatural roll. These results facilitate physical understanding of the large-scale cellular flows observed in the numerical simulations at different values of
ϕ
.
“…Closed sites are typically fault bounded and do not allow compensation of pressure changes by brine migration. Therefore, the volume of CO 2 vapour in a closed system remains essentially constant over time and consequently CO 2 dissolution reduces the pressure in the vapour phase (Akhbari & Hesse 2017). This leads to a decline of the aqueous CO 2 concentration beneath the gas-water contact and therefore reduces the density difference driving convective dissolution.…”
Section: Introductionmentioning
confidence: 99%
“…Here we show that the pressure drop in the gas can limit CO 2 dissolution long before saturation of the brine becomes a limiting factor. These negative feedbacks in closed systems are common in experiments on CO 2 dissolution (Farajzadeh et al 2009;Moghaddam et al 2012;Mojtaba et al 2014;Shi et al 2017) and in some natural CO 2 reservoirs that serve as analogs for geological CO 2 storage (Akhbari & Hesse 2017). Engineered geological storage sites are typically selected such that CO 2 is supercritical to maximise the storage capacity (Orr 2009).…”
Motivated by geological carbon dioxide (CO 2 ) storage, many recent studies have investigated the fluid dynamics of solutal convection in porous media. Here we study the convective dissolution of CO 2 in a closed system, where the pressure in the gas declines as convection proceeds. This introduces a negative feedback that reduces the convective dissolution rate even before the brine becomes saturated. We analyse the case of an ideal gas with a solubility given by Henry's law, in the limits of very low and very high Rayleigh numbers. The equilibrium state in this system is determined by the dimensionless dissolution capacity, Π, which gives the fraction of the gas that can be dissolved into the underlying brine. Analytic approximations of the pure diffusion problem with Π > 0, show that the diffusive base state is no longer self-similar and that diffusive mass transfer declines rapidly with time. Direct numerical simulations at high Rayleigh numbers show that no constant flux regime exists for Π > 0; nevertheless, the quantity F/C 2 s remains constant, where F is the dissolution flux and C s is the dissolved concentration at the top of the domain. Simple mathematical models are developed to predict the evolution of C s and F for high-Rayleigh-number convection in a closed system. The negative feedback that limits convection in closed systems may explain the persistence of natural CO 2 accumulations over millennial timescales.
“…Likewise, the simulations included only pure water and methane gas, but the salinity of brine at the site (Nuclear Waste Management Organization 2011) could have significant effects on gas solubility (Duan & Mao 2006). Further analyses of the effects of brine-relevant gas solubility on multiphase methane and pressure at the site would therefore also be beneficial (Akhbari & Hesse 2017). Due to the common co-occurrence of gas phase and underpressures in other sedimentary basins around the world (Vinard 1988;Corbet & Bethke 1992;Law & Spencer 1998), examples of which can be found in both glaciated (Masters 1979) and nonglaciated (Davis 1984) regions, improved understanding of the Bruce site may inform efforts to understand those systems as well.…”
Hydraulic testing has revealed dramatic underpressures in Paleozoic shales and carbonates at the Bruce nuclear site in Ontario. Although evidence from both laboratory and field studies suggests that a small amount of gas-phase methane could be present in the shale, previous studies examining causal linkages between the gas phase and the underpressure have been inconclusive. To better elucidate processes in such a system, we used a highly simplified 1D representation of the site to test, by using iTOUGH2-EOS7C, the effects of various factors on the evolution of gas-phase methane and pressures within the system. Heterogeneity was represented by three stratigraphic regions with slightly different capillary pressure characteristics and, in one case, three thin distinct zones with very different characteristics. Underpressure occurred only when gas pressures set as an initial condition required it, and even in this case it was geologically short-lived. We conclude that the presence of multiple fluid phases is unlikely to explain the underpressure at the site; we suggest that the influence of gasphase methane on porewater flow is minimal. This is consistent with prior conceptualizations of the underpressured section as a thick aquiclude, in which solute transport occurs extremely slowly, bounded by aquifers of significantly higher permeability.
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