Modelling Pore Occupancies in Three-phase Displacements from Micro-CT Images Using a Physics-Based Theory of Wettability and Miscibility Conditions

Abstract Advanced digital rock technology using X-ray microtomography (micro-CT) has been applied to investigate three-phase pore occupancies in rock samples. These three-phase experiments involved different injection sequences in water-wet, oil-wet and mixed-wet rocks under immiscible and near miscible conditions using carbon dioxide or nitrogen as injected gases. In this work, the process-based theory of van Dijke et al ., which has been previously used in both capillary bundle (CB) and 3D-lattice pore network models (PNM), is applied to simulate all the available published three-phase pore occupancy data. The predicted three-phase pore occupancies from the CB model are compared to the experimental results. The three-phase theory first uses the physical parameters as reported by the original authors; namely, the three values of interfacial tension (σ ow , σ go , and σ gw ), wetting conditions and the distribution of oil–water contact angle where a single contact angle is assigned to each pore. However, there are some uncertainties in these quantities, and to achieve a good match some reasonable adjustment of the input data is usually required. For water-wet systems, the best agreement with the measured pore occupancy is achieved with only minor parameter adjustments: for example, a change of 2 mN/m in gas-oil interfacial tension and a decrease in gas–water interfacial tensions to represent true three-phase equilibrium conditions. For oil-wet and mixed-wet systems, adjusted contact angle distributions, within the experimental uncertainty, are also required to match the data. Both the experimental results and modelling predictions show that three-phase displacements are the same at immiscible (gas-oil interfacial tensions of around 10 mN/m or more) and near-miscible (gas-oil interfacial tensions of approximately 1 mN/m) conditions for water-wet cases, while in oil-wet systems, miscibility affects the wetting order of gas and water. Water becomes the most non-wetting phase at near-miscible conditions and gas is intermediate-wet. The model developed in this work also helps (i) to interpret the physical processes in the experiment and (ii) to determine the likely equilibrium values of interfacial tension and contact angles.

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Publication Details

Journal
Transport in Porous Media
Published
2025-08-18
DOI
https://doi.org/10.1007/s11242-025-02208-x
Citations
2
Primary Topic
Enhanced Oil Recovery Techniques
Type
article
Field-Weighted Citation Impact
2.29

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article

Modelling Pore Occupancies in Three-phase Displacements from Micro-CT Images Using a Physics-Based Theory of Wettability and Miscibility Conditions

Ken Stuart Sorbie, Arne Skauge, Saba Mahmoudvand, Martin J. Blunt
2 citations
Transport in Porous Media
Enhanced Oil Recovery Techniques
2.29
article

Modelling Pore Occupancies in Three-phase Displacements from Micro-CT Images Using a Physics-Based Theory of Wettability and Miscibility Conditions

Ken Stuart Sorbie, Arne Skauge, Saba Mahmoudvand, Martin J. Blunt
article en
2 citations

Abstract

Abstract Advanced digital rock technology using X-ray microtomography (micro-CT) has been applied to investigate three-phase pore occupancies in rock samples. These three-phase experiments involved different injection sequences in water-wet, oil-wet and mixed-wet rocks under immiscible and near miscible conditions using carbon dioxide or nitrogen as injected gases. In this work, the process-based theory of van Dijke et al ., which has been previously used in both capillary bundle (CB) and 3D-lattice pore network models (PNM), is applied to simulate all the available published three-phase pore occupancy data. The predicted three-phase pore occupancies from the CB model are compared to the experimental results. The three-phase theory first uses the physical parameters as reported by the original authors; namely, the three values of interfacial tension (σ ow , σ go , and σ gw ), wetting conditions and the distribution of oil–water contact angle where a single contact angle is assigned to each pore. However, there are some uncertainties in these quantities, and to achieve a good match some reasonable adjustment of the input data is usually required. For water-wet systems, the best agreement with the measured pore occupancy is achieved with only minor parameter adjustments: for example, a change of 2 mN/m in gas-oil interfacial tension and a decrease in gas–water interfacial tensions to represent true three-phase equilibrium conditions. For oil-wet and mixed-wet systems, adjusted contact angle distributions, within the experimental uncertainty, are also required to match the data. Both the experimental results and modelling predictions show that three-phase displacements are the same at immiscible (gas-oil interfacial tensions of around 10 mN/m or more) and near-miscible (gas-oil interfacial tensions of approximately 1 mN/m) conditions for water-wet cases, while in oil-wet systems, miscibility affects the wetting order of gas and water. Water becomes the most non-wetting phase at near-miscible conditions and gas is intermediate-wet. The model developed in this work also helps (i) to interpret the physical processes in the experiment and (ii) to determine the likely equilibrium values of interfacial tension and contact angles.

Transport in Porous MediaVol. 152(10)
Heriot-Watt University (GB), Imperial College London (GB)
Energi Simulation
Openalex Percentile: Top 11%
Enhanced Oil Recovery Techniques
2.29
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