scholarly journals Capillary Desaturation in Unconsolidated Beads

1953 ◽  
Vol 5 (08) ◽  
pp. 197-202 ◽  
Author(s):  
F.T. Bethel ◽  
John C. Calhoun
1979 ◽  
Vol 19 (06) ◽  
pp. 357-368 ◽  
Author(s):  
G.A. Pope ◽  
Ben Wang ◽  
Kerming Tsaur

Abstract The compositional simulator of Pope and Nelson has been extended to include a number of additional effects. The efficiency of the oil displacement has been calculated as a function of slug size, polymer drive size, surfactant and oil concentrations in the slug, slug/oil bank and drive/slug mobility ratios, surfactant and polymer absorption, interfacial tension (IFT), phase type, binodal curves, plait point location, capillary desaturation curves for each point location, capillary desaturation curves for each phase, relative permeabilities, waterflood residuals, phase, relative permeabilities, waterflood residuals, dispersion, electrolyte gradient, and amount of surfactant injected. High-concentration slugs in a Type II (+) (or plait point left) phase environment were found to be less dependent on low IFT than low-concentration slugs or slugs in a type II (-) phase environment. For the Type II (-) case, oil phase environment. For the Type II (-) case, oil recovery is not sensitive to plait point location. However, the best oil recovery for a given amount of injected surfactant occurs where a salinity higher than optimal exists downstream of the slug and a salinity lower than optimal exists upstream of the slug (in the polymer drive) and the slug itself traverses as much of the reservoir as possible in the low-tension Type III environment. The low final salinity promotes low final retention of surfactant. For the cases studied, the salinity, surfactant concentration, oil concentration, and polymer concentration of the slug itself then made relatively little difference. Introduction Several authors have examined one-dimensional simulation of surfactant flooding and the various complex compositional effects that occur during the displacement of oil with surfactants and polymers. Nelson and Pope presented laboratory results showing the importance of the Type III phase environment and how oil recovery can result from mechanisms other than low IFT. Actually, several key phenomena affecting oil recovery are strongly coupled and need to be considered simultaneously both to understand and to simulate the process. The simulator of Pope and Nelson was a first attempt to model these effects, which include IFT, phase behavior, fractional flow, adsorption, and polymer properties as a function of electrolyte. Ion exchange properties as a function of electrolyte. Ion exchange has been shown to have an important impact on the process as well, since the electrolyte environment process as well, since the electrolyte environment affects many of the most important fluid properties involved. Pope and Nelson have shown how the displacement of oil is "miscible-like" under certain conditions, even when dispersion and adsorption are considered and small slugs are used. However, to be practical, a very carefully designed electrolyte practical, a very carefully designed electrolyte gradient must exist (or some other equivalent gradient of another variable such as surfactant molecular weight, alcohol, etc.). Here we continue the investigation of these process variables by presenting results of a sensitivity study. Both presenting results of a sensitivity study. Both water and oil-rich surfactant slug cases are simulated. Model Changes Pope and Nelson presented a description of the Pope and Nelson presented a description of the original simulator. Several changes that have been made will be discussed briefly. The IFT functions are now those proposed by Healy and Reed. ....... (1) ....... (2) SPEJ P. 357


2015 ◽  
Vol 51 (10) ◽  
pp. 8517-8528 ◽  
Author(s):  
Antonio Rodríguez de Castro ◽  
Nima Shokri ◽  
Nikolaos Karadimitriou ◽  
Mart Oostrom ◽  
Vahid Joekar‐Niasar

SPE Journal ◽  
2018 ◽  
Vol 23 (03) ◽  
pp. 788-802 ◽  
Author(s):  
B. I. AlQuaimi ◽  
W. R. Rossen

Summary The displacement of a nonwetting phase by a wetting phase is characterized by the capillary number. Different forms of capillary number have been used in the literature for flow in porous media. A capillary number for a single rock fracture has been defined in the literature, using the mean aperture to characterize the trapping and mobilization in a fracture. We propose a new capillary-number definition for fractures that incorporates geometrical characterization of the fracture, dependent on the force balance on a trapped ganglion. The new definition is validated with laboratory experiments using five distinctive model fractures. The model fractures are made of glass plates, with a wide variety of hydraulic apertures, degrees of roughness, and correlation lengths of the roughness. The fracture surfaces were characterized in detail and statistically analyzed. The aperture distribution of each model fracture was represented as a 2D network of pore bodies connected by throats. The hydraulic aperture of each model fracture was measured experimentally. Capillary desaturation curves (CDCs) were generated experimentally using water/air in forced imbibition. The transparent nature of the system permits us to determine the residual air saturation as a function of pressure gradient from the captured images. The residual nonwetting saturation/capillary-number relationship obtained from different fractures varying in aperture and roughness can be represented approximately by a single curve in terms of the new definition of the capillary number. They do not fit a single trend using the conventional definition of the capillary number.


2015 ◽  
Vol 112 (7) ◽  
pp. 1947-1952 ◽  
Author(s):  
Tannaz Pak ◽  
Ian B. Butler ◽  
Sebastian Geiger ◽  
Marinus I. J. van Dijke ◽  
Ken S. Sorbie

Using X-ray computed microtomography, we have visualized and quantified the in situ structure of a trapped nonwetting phase (oil) in a highly heterogeneous carbonate rock after injecting a wetting phase (brine) at low and high capillary numbers. We imaged the process of capillary desaturation in 3D and demonstrated its impacts on the trapped nonwetting phase cluster size distribution. We have identified a previously unidentified pore-scale event during capillary desaturation. This pore-scale event, described as droplet fragmentation of the nonwetting phase, occurs in larger pores. It increases volumetric production of the nonwetting phase after capillary trapping and enlarges the fluid−fluid interface, which can enhance mass transfer between the phases. Droplet fragmentation therefore has implications for a range of multiphase flow processes in natural and engineered porous media with complex heterogeneous pore spaces.


2020 ◽  
Vol 144 ◽  
pp. 103702 ◽  
Author(s):  
Abdelhalim I. A. Mohamed ◽  
Mahdi Khishvand ◽  
Mohammad Piri

2017 ◽  
Vol 204 ◽  
pp. 57-65 ◽  
Author(s):  
Thomas Robert ◽  
Richard Martel ◽  
René Lefebvre ◽  
Jean-Marc Lauzon ◽  
Annie Morin

2021 ◽  
Author(s):  
Amaar Siyal ◽  
Khurshed Rahimov ◽  
Waleed AlAmeri ◽  
Emad W. Al-Shalabi

Abstract Different enhanced oil recovery (EOR) methods are usually applied to target remaining oil saturation in a reservoir after both conventional primary and secondary recovery stages. The remaining oil in the reservoir is classified into capillary trapped residual oil and unswept /bypassed oil. Mobilizing the residual oil in the reservoir is usually achieved through either decreasing the capillary forces and/or increasing the viscous or gravitational forces. The recovery of the microscopically trapped residual oil is mainly studied using capillary desaturation curve (CDC). Hence, a fundamental understanding of the CDC is needed for optimizing the design and application of different EOR methods in both sandstone and carbonate reservoirs. For sandstone reservoirs, especially water-water rocks, determining the residual oil saturation and generating CDC has been widely studied and documented in literature. On the other hand, very few studies have been conducted on carbonate rocks and less data is available. Therefore, this paper provides a comprehensive review of several important research studies published on CDC over the past few decades for both sandstone and carbonate reservoirs. We critically analyzed and discussed theses CDC studies based on capillary number, Bond number, and trapping number ranges. The effect of different factors on CDC were further investigated including interfacial tension, heterogeneity, permeability, and wettability. This comparative review shows that capillary desaturation curves in carbonates are shallower as opposed to these in sandstones. This is due to different factors such as the presence of high fracture density, presence of micropores, large pore size distribution, mixed-to-oil wetting nature, high permeability, and heterogeneity. In general, the critical capillary number reported in literature for sandstone rocks is in the range of 10−5 to 10−2. However, for carbonate rocks, that number ranges between 10−8 and 10−5. In addition, the wettability has been shown to have a major effect on the shape of CDC in both sandstone and carbonate rocks; different CDCs have been reported for water-wet, mixed-wet, and oil-wet rocks. The CDC shape is broader and the capillary number values are higher in oil-wet rocks compared to mixed-wet and water-wet rocks. This study provides a comprehensive and comparative analysis of CDC in both sandstone and carbonate rocks, which serves as a guide in understanding different CDCs and hence, better screening of different EOR methods for different types of reservoirs.


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