Issue 67, 2018, Issue in Progress

Interfacial tension and CO2 diffusion coefficients for a CO2 + water and n-decane system at pressures of 10 to 160 bar

Abstract

The objective of this study is to address the influence of different CO2 phases and degrees of CO2 saturation on the interfacial tension and the diffusion of CO2 into a hydrocarbon drop. Axisymmetric drop shape analysis on a pendant drop was used to carry out experiments in a pressure range of 10 to 160 bar and temperatures of 25 °C, 35 °C, and 45 °C, thus covering the gaseous, liquid, and supercritical phases of CO2. A numerical model that estimates the diffusion coefficient of CO2 in the hydrocarbon was developed. The IFT between the carbonated water and the hydrocarbon increases with pressure in the gaseous phase of CO2 and decreases in the liquid and supercritical CO2 phases. Interestingly, when the pressure was increased above 120 bar, the IFT did not change (decrease); this indicates that above this pressure, complete miscibility may not be achieved for this system, as indicated by the stable IFT. From the results, it can be concluded that the maximum IFT, maximum density decrease, and minimum diffusion coefficient occurred at pressures near to and below the phase change pressure of CO2 (64 bar at 25 °C and 74 bar at 35 °C and 45 °C). Both CO2–water–hydrocarbon and CW–hydrocarbon systems show the same trends; however, there were significant differences in the CO2 mass transfer rate and the concentration gradient.

Graphical abstract: Interfacial tension and CO2 diffusion coefficients for a CO2 + water and n-decane system at pressures of 10 to 160 bar

Supplementary files

Article information

Article type
Paper
Submitted
29 Apr 2018
Accepted
31 Oct 2018
First published
14 Nov 2018
This article is Open Access
Creative Commons BY-NC license

RSC Adv., 2018,8, 38351-38362

Interfacial tension and CO2 diffusion coefficients for a CO2 + water and n-decane system at pressures of 10 to 160 bar

N. Bagalkot and A. A. Hamouda, RSC Adv., 2018, 8, 38351 DOI: 10.1039/C8RA03690J

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