Predicting PVT data for CO2–brine mixtures for black-oil simulation of CO2 geological storage
Introduction
The sequestration of anthropogenic CO2 into geological formations has been considered as a potential method to mitigate climate change. Accurate evaluation of the capacity of a saline aquifer for CO2 sequestration, and the fate of the injected fluids in sedimentary basins needs precise representation of brine and CO2 PVT data (Adams and Bachu, 2002, Bachu and Adams, 2003). Experimental data reported in the literature show that the density of an aqueous solution of CO2 could be slightly greater than that of pure water (Blair and Quinn, 1968, Sayegh and Najman, 1987, Hnedovsky et al., 1996). This density variation might cause free convection motion, which in turn causes increased dissolution over a larger distance and shorter time scales compared to pure diffusive flow (Lindeberg and Wessel-Berg, 1996, Ennis-King and Paterson, 2003, Ennis-King and Paterson, 2005, Ennis-King et al., 2005, Hassanzadeh et al., 2005). Therefore, accurate description of the thermodynamic and transport properties of CO2 and brine are very important for evaluating the capacity of saline aquifers to sequester CO2 by a solubility trapping mechanism.
In the petroleum industry, compositional reservoir simulators use EOS thermodynamic models to calculate the phase equilibrium properties of fluid mixtures (Chang et al., 1998). Although these kinds of thermodynamic models are well suited for compositional modeling of enhanced oil recovery (EOR) processes, such as miscible gas injection, the disadvantage of such models for the specific case of large-scale flow simulation of geological CO2 storage in aquifers is that they represent computational “overkill” and are inappropriately expensive. Therefore, it would be helpful if we were able to use a simple thermodynamic model that can predict the CO2–brine equilibrium properties accurately with less computational overhead. Indeed, there are a large number of experimental equilibrium data on the CO2–brine system that have been used to develop correlations and tune the equations of state for CO2 and water under subsurface conditions. Such experimental and EOS data are used in this paper to develop a black-oil PVT module needed for flow simulation geological storage of CO2 in saline aquifers. The novelty of this work is in presenting a PVT module for converting compositional data into black-oil that provides accurate PVT data required for black-oil flow simulation of CO2 storage in saline aquifers. The black-oil PVT module developed in this work is validated with experimental data available in the literature. Furthermore, our numerical flow simulations of CO2 storage reveal that the black-oil simulation approach is computationally more efficient than the compositional approach. The accuracy in prediction of CO2–brine PVT properties and superior computational efficiency encourages application of black-oil simulation approach for large-scale geological storage of CO2 in saline aquifers.
The thermodynamic model used in this work is based on a combination of the Duan and Sun (2003) and Spycher et al. (2003) models. Similar models have recently appeared in the literature (Spycher and Pruess, 2005, Portier and Rochelle, 2005, Duan et al., 2006). In this paper, in addition to presentation of our thermodynamic module, we use it to generate CO2–brine PVT properties as required for black-oil flow simulation. For completeness, we also present the correlations of transport properties of the CO2 and brine system required for black-oil reservoir simulation.
This paper is organized as follows. First a brief review of the literature on thermodynamic modeling of CO2–brine equilibrium is presented. Then, the thermodynamic model used in this study is described and its results are compared with experimental data available in the literature. This is followed by the main contribution of the paper; representation of the CO2–brine PVT properties suitable for black-oil simulation and a comparison of black-oil and compositional simulator computational performances for simulation of CO2 injection into saline aquifers.
Section snippets
Review of CO2–brine solubility data
The CO2–water equilibrium phenomenon has been studied extensively in literature. The interested reader might consult more exhaustive reviews from Diamond and Akinfiev (2003), Duan and Sun (2003), and Spycher et al. (2003) among others. In this section, a brief review of some of the studies is presented. Wiebe and Gaddy (1939) and Wiebe (1941) reported experimental solubility of CO2 in water at temperatures up to 100 °C and pressures up to 700 atm. Dodds et al. (1956) have used available
Thermodynamic model
From the definition of fugacity, we have:where f denotes fugacity; φ fugacity coefficient; p total pressure; y is the mole fraction in the gaseous phase. At equilibrium, the following equilibrium relationship holds (Spycher et al., 2003):where κ parameters are true equilibrium constants and a is the activity of a component in the aqueous phase. The κ parameters are functions of pressure and temperature as given by the following expression (Spycher
Comparison with experimental data
Chang et al. (1998), Diamond and Akinfiev (2003), Duan and Sun (2003), Spycher et al. (2003), Spycher and Pruess (2005), Portier and Rochelle (2005), and Duan et al. (2006) reviewed and used CO2–brine mixture data available in the literature to develop their solubility model. In this section, we compare the calculated CO2–water properties with such experimental data from the literature. These experimental data are taken from King et al. (1992), Wiebe and Gaddy, 1939, Wiebe and Gaddy, 1940,
Representation of CO2–brine equations of state predictions in a black-oil simulator
The choice of the fluid model is very important in any flow simulation including simulation of CO2 storage in saline aquifers. Black-oil flow simulators have been used for modeling fluid flow in petroleum reservoirs, when the reservoir fluids can be lumped into three components, oil, gas and water (Aziz and Settari, 1979). In such simulators, these three components can be partitioned in three phases generically called oil, gas and water. In this system, the gas component is usually partitioned
Performance comparison of black-oil and compositional simulations
Compositional reservoir simulators are well known to be more time consuming than black-oil simulators. This is due to the fact that compositional simulators perform frequent phase equilibrium and flash calculations at each time step. Furthermore, the formulation in compositional simulators is more complicated. Very often, this results in a larger number of time-steps used by the compositional simulator. Compositional simulators may have stability limitations resulting from the time
Discussion
This paper proposes the use of black-oil models for simulation studies of CO2 storage in deep aquifers, and presents a simple and efficient algorithm for computing the necessary PVT data. For this purpose, the gaseous phase in the black-oil formulation was used to represent the super-critical CO2 phase. This is appropriate for most scenarios of geological storage of CO2, where the aquifer depth is more than 800–1000 m and the pressure and temperature conditions are above the CO2 critical point.
Summary and conclusions
Flow modeling of CO2 sequestration in saline aquifers has been treated in the literature since the early 1990s. Accurate evaluation of capacity of a saline aquifer to sequester CO2 by solubility trapping needs precise representation of PVT data for the CO2–brine system. Compositional reservoir simulators that account for complex phase behavior and very compositionally dependent systems are computationally expensive compared to traditional black-oil simulators. Although such compositional models
Acknowledgements
The authors would like to thank Nicolas Spycher for his review and constructive comments. Useful comments from the journal associate editor Stefan Bachu and two anonymous reviewers that improved the original version of the paper are acknowledged. The financial support for this work was provided by the National Science and Engineering Research Council of Canada (NSERC) and the Alberta Department of Energy. This support is gratefully acknowledged. The first author also thanks the National Iranian
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