Lanlan Jiang

Doctoral Degree

Dalian University of Technology

Personal Information

Gender:Female
Business Address:Room No.609,School of Energy and Power Engineering
E-Mail:lanlan@dlut.edu.cn

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Dynamic stability characteristics of fluid flow in CO2 miscible displacements in porous media

Date of Publication:2015-01-01 Hits:

Indexed by:期刊论文
Date of Publication:2015-01-01
Journal:RSC ADVANCES
Included Journals:SCIE、EI、Scopus
Volume:5
Issue:44
Page Number:34839-34853
ISSN No.:2046-2069
Abstract:The dynamic characteristics of fluid flow are important in miscible displacement processes in carbon dioxide enhanced oil recovery (CO2-EOR) projects. And the stability of the in situ mixing zone greatly influences the oil recovery factor, which deserves further research. We investigated CO2 miscible displacement processes using magnetic resonance imaging (MRI) apparatus. The CO2 miscible displacement flows were performed at a low injection rate of 0.1 ml min(-1) with reservoir conditions of 8.5 to 9.5 MPa and 37.8 degrees C. The oil saturation evolution, the length of the in situ mixing zone, and the mixing-frontal velocity and CO2-frontal velocity were quantified. The experimental results showed that the residual oil saturation decreased with pressure and the mixing zone length was independent of pressure. The mixing-frontal velocity and the CO2-frontal velocity were nearly the same and increased with pressure. The critical velocity of the CO2/n-decane (CO2/nC(10)) system was 1.105 x 10(-5) m s(-1). Although the whole mixing zone length had no obvious change with pressure, a higher pressure compressed the mixing zone and led to an unstable mixing front above the critical velocity. The longitudinal dispersion coefficient was calculated by fitting the experimental data with an error function, which had no obvious change with pressure. Additionally, a three-dimensional lattice-Boltzmann method (LBM) was used to simulate pore-scale miscible fluid flows in upward vertical displacements. A front fingering occurred at a low kinematic viscosity ratio (nu(Co2) : nu(o) = 1 : 1). At a large kinematic viscosity ratio (nu(Co2) : nu(o) = 1 : 15), the high kinematic viscous oil restrained the buoyancy of supercritical CO2, but also impeded the displacement with a pore-scale backflow which might lead to a low oil recovery factor.