energies
Article
CO
2
Convective Dissolution in Oil-Saturated Unconsolidated
Porous Media at Reservoir Conditions
Widuramina Amarasinghe
1,2,
*, Ingebret Fjelde
1
, Nils Giske
1
and Ying Guo
1,2
Citation: Amarasinghe, W.; Fjelde, I.;
Giske, N.; Guo, Y. CO
2
Convective
Dissolution in Oil-Saturated
Unconsolidated Porous Media at
Reservoir Conditions. Energies 2021,
14, 233. https://doi.org/10.3390/
en14010233
Received: 9 December 2020
Accepted: 30 December 2020
Published: 4 January 2021
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4.0/).
1
NORCE Norwegian Research Center AS, P.O. Box 8046, 4068 Stavanger, Norway; infj@norceresearch.no (I.F.);
nigi@norceresearch.no (N.G.); yigu@norceresearch.no (Y.G.)
2
Department of Energy Resources, University of Stavanger, P.O. Box 8600, 4036 Stavanger, Norway
* Correspondence: widuramina@norceresearch.no
Abstract: During CO
2
storage, CO
2
plume mixes with the water and oil present at the reservoir,
initiated by diffusion followed by a density gradient that leads to a convective flow. Studies are
available where CO
2
convective mixing have been studied in water phase but limited in oil phase.
This study was conducted to reach this gap, and experiments were conducted in a vertically packed
3-dimensional column with oil-saturated unconsolidated porous media at 100 bar and 50
◦
C (rep-
resentative of reservoir pressure and temperature conditions). N-Decane and crude oil were used
as oils, and glass beads as porous media. A bromothymol blue water solution-filled sapphire cell
connected at the bottom of the column was used to monitor the CO
2
breakthrough. With the increase
of the Rayleigh number, the CO
2
transport rate in n-decane was found to increase as a function of a
second order polynomial. Ra number vs. dimensionless time τ had a power relationship in the form
of Ra = c × τ
−n
. The overall pressure decay was faster in n-decane compared to crude oil for similar
permeability (4 D), and the crude oil had a breakthrough time three times slower than in n-decane.
The results were compared with similar experiments that have been carried out using water.
Keywords: convection; porous media; reservoir conditions; oil; CO
2
dissolution; 3-dimensional
column
1. Introduction
CO
2
storage is a commonly considered topic when it comes to climate change miti-
gation. Injection of CO
2
to active and abandoned oil and gas fields is a well-discovered
solution for a viable utilization of CO
2
due to its commercial benefits of enhancing the oil
recovery (EOR) as well as achieving permanent CO
2
storage [1,2]. During CO
2
injection
into existing oil fields for EOR, the added CO
2
will swell and reduce the viscosity and will
lead to an increase of the oil recovery percentage [3,4]. EOR for CO
2
utilization can also
reduce a significant cost of the whole CCS value chain [5–7].
When CO
2
is injected into the oil fields, a CO
2
plume will usually develop above
the fluid phases inside the porous media due to the low density of CO
2
compared to
the density of the reservoir fluids, as shown in Figure 1 [8]. Initially, this CO
2
plume
mixes with the oil and water phases present in the reservoir mainly due to diffusion.
The mixing process creates a density gradient (e.g., increase the density of oil). This
phenomenon leads to a convective flow, which will accelerate the CO
2
mixing and mass
transfer and will significantly enhance the underground CO
2
storage rate as well as the oil
production [7,9–11].
It is essential to know the behavior of the CO
2
plume in the reservoir along with how
CO
2
will dissolve convectively into the oil phase. This helps to understand how CO
2
will be
transported during long-term storage after injection for storage and EOR. The convectively
driven dissolution has been extensively studied for accelerated CO
2
dissolution in saline
water for CO
2
storage in 2-dimensional (2-dim) Hele-Shaw experimental setups [12–18] and
using 3-dimensional (3-dim) confined experimental setups [19–24]. An extensive review
Energies 2021, 14, 233. https://doi.org/10.3390/en14010233 https://www.mdpi.com/journal/energies