4.4 Article

Long-Term Redistribution of Residual Gas Due to Non-convective Transport in the Aqueous Phase

Journal

TRANSPORT IN POROUS MEDIA
Volume 141, Issue 1, Pages 231-253

Publisher

SPRINGER
DOI: 10.1007/s11242-021-01722-y

Keywords

Residual trapping; Thermodynamic equilibrium; Non-convective transport; CO2 sequestration

Funding

  1. Global Climate and Energy Project (GCEP)
  2. Stanford Center for Carbon Storage (SCCS)
  3. Center of Nanoscale Controls on Geologic CO2 (NCGC) - U.S. Department of Energy [DE-AC02-05CH11231]

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Geological CO2 sequestration is an effective way to permanently trap greenhouse gas emissions underground. In addition to convective mixing, non-convective transport plays a role in redistributing trapped CO2, with mechanisms such as molecular diffusion and sedimentation. Despite being slow, non-convective transport can cause localized accumulation and potentially remobilize trapped gas.
Geological CO2 sequestration is an effective approach to mitigate greenhouse gas emissions by permanently trapping CO2 in the subsurface. A large portion of injected CO2 is trapped by capillary forces in pores and eventually dissolves into the reservoir brine due to convective mixing to achieve permanent entrapment. In regions where convective mixing is slow, non-convective transport can play an important role in redistributing residually trapped CO2, but the mechanisms and timescales for redistribution have yet to be explored thoroughly. In previous work, we have shown that capillary pressure difference among residually trapped gas ganglia can induce Ostwald ripening, thereby redistributing the separate-phase gas through diffusion despite the gas phase remaining trapped over the entire course of equilibration. In this study, we show from a thermodynamic point of view that other natural gradients in geologic formations- hydrostatic pressure, geothermal gradients and capillary heterogeneity-can also redistribute CO2 by non-convective transport. Mechanisms for resulting non-convective transport include molecular diffusion, the sedimentation effect and potentially the Soret effect. Results show that hydrostatic pressure dominates redistribution such that the separate-phase gas is transported upward through molecular diffusion and accumulates under the seal at the steady state. A typical timescale for gas phase redistribution is 10(5) years/m; for a 100-m-thick formation, redistribution is complete after similar to 10(7) years. Although non-convective transport is an extremely slow process, it causes local accumulation of the gas phase and in some settings may remobilize the trapped gas phase.

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