1. Introduction
The need for new hydrocarbon resources led to the unconventional reservoir boom in the early 2000s. Horizontal drilling and multi-stage hydraulic fracturing have enabled production from ultra-tight formations; however, the recovery factor remains low in these deposits, typically around 5–10% [
1,
2]. The low recovery rates have prompted researchers and the industry to explore the possibility of enhanced oil recovery (EOR) methods, which are similar to conventional reservoirs.
Simultaneously, the need to manage greenhouse gas emissions and the decarbonization of the energy industry are fueling the development of carbon capture, utilization, and storage (CCUS) projects. CCUS refers to several technologies that aim to capture carbon dioxide (CO
2) from processes (e.g., fossil fuel power plants), pressurize it, and eventually either neutralize it through added-value products or store it underground [
3,
4]. CO
2-EOR has been identified as one example of CO
2 utilization [
5,
6]. The combination of CO
2-EOR and CCUS is referred to as CO
2-EOR+ [
5].
CO
2-EOR+ (this term is used interchangeably with CO
2-EOR in this work) is an attractive option for the energy industry as it results in improved recovery (i.e., financial gain) and a lower carbon footprint for the produced oil. It is estimated that oil production through CO
2-EOR+ results in a 63% lower carbon footprint per barrel of oil [
4]. For CO
2-EOR+ to contribute to emission reduction, the CO
2 must come from anthropogenic sources.
EOR studies on shales have typically been limited to lab tests and numerical simulations, with few field trials. Most studies have considered the huff-n-puff scheme for their investigation. In huff-n-puff, CO
2 or other gasses are injected into the well for a certain duration, then the well is shut down for a given time interval, and finally, the same well is opened for production. In this approach, the fractured reservoir is soaked in the injected fluid. Diffusion (which is driven by the concentration gradient) is expected to be the dominant mode of transport under a waning pressure gradient [
7]. EOR through huff-n-puff is affected by several parameters, such as injection plan, gas injection rate and volume, pressure, cycle time, reservoir heterogeneity, pore space, and shale characteristics, some of which are design parameters whereas others are simply reservoir properties.
Among the lab studies, Hawthorne et al. [
7] studied the use of CO
2-EOR on 51 shale samples from the Bakken Petroleum System in the US. The shale samples were exposed to supercritical CO
2 for 24 h under reservoir conditions. Significant oil was recovered from the Lower and Upper Bakken (hereafter LB and UB) samples, despite a median pore throat radius of 3.5 nm. The authors’ analysis of the mineralogical composition of the samples indicated that these parameters were not relevant for predicting the recovery factor. In a later study, Hawthorne and Miller [
8] investigated the impacts of the injection of various gases under different pressures on the produced hydrocarbon. CO
2, produced gas (natural gas), and several pure hydrocarbons were tested as potential EOR injections. Their results indicated that CO
2 could dissolve heavier hydrocarbon components better than CH
4 and produced gas but fell short compared to propane and ethane.
Jin et al. [
9,
10] used core plugs from the Bakken Formation to study oil recovery under the diffusive regime in a fractured reservoir. The apparatus that they used, along with the low injection rate, allowed for the neglecting of convective and pressure-driven flows. The Middle Bakken (MB) samples showed very high recovery factors (>90%), while the shale samples had recovery factors of around 60%. An analysis of the importance of the parameters indicated that the total organic carbon (TOC) content was an important parameter in the oil recovery from shales, while the porosity and permeability had little impact. The authors argued that kerogen-hosted pores were smaller than matrix pores, in addition to their oil-wet surface, which made oil extraction from these pores much harder for CO
2. Therefore, high TOC content may be detrimental to CO
2-EOR efforts in shales.
In terms of recovery mechanisms, different mechanisms have been proposed for gas injection in shales, e.g., molecular diffusion [
11,
12,
13], repressurization [
14], swelling, capillary pressure reduction, multi-contact miscible displacement [
10], and any combination of these methods. In conventional systems, CO
2 penetrates the matrix and causes swelling, viscosity reduction or sweeping of the in-place oil [
15]. In shales, the concentration gradient-driven diffusion of hydrocarbons from the interstitial pore spaces in the rock to the surface and into the bulk-injected fluid in the fractures is considered to be the main recovery mechanism [
7,
8,
16,
17]. The minimum miscibility pressure (MMP) may not be as important in CO
2-EOR in shales as it is in conventional systems.
According to Mahzari et al. [
18], in conventional reservoirs, the injected CO
2 is in direct contact with the oil in large pores. A two-way diffusion takes place in this case, in which a mass transfer occurs in both phases [
18]. In fractured shales, the CO
2 is injected into the fractures and a one-way mass transfer is expected at the interface of the fracture and rock matrix. The unidirectional mass transfer causes CO
2 to diffuse into the oil phase, causing swelling and viscosity reduction [
18,
19]. While the pressure-driven transfer of CO
2 into the matrix is also expected (along with some inward hydrocarbon movement), the swelling and viscosity reduction are the primary causes of oil recovery.
Additionally, the diffusion of CO
2 into the resident oil also results in the liberation of light components [
18]. The liberated components form a new gaseous phase that remains immobile up to a critical concentration (15% according to Mahzari et al. [
18]). The liberation of the light components can result in significant swelling, which ultimately improves recovery. The numerical modeling of CO
2-EOR in Bakken shale by Mahzari et al. [
18], as well as the five-step recovery process proposed by Hawthorne et al. [
19], supports the use of EOR through diffusion (driven by concentration gradient). The experiments by Li et al. [
20] on shales from the Jianghan oilfield, Jianghan Basin, also indicated the preferential tendency of CO
2 to recover lighter hydrocarbon, which can be caused by the above mechanism.
When we assume a diffusion-dominant model for the EOR mechanism in shales, a one-way mass transfer (CO
2 diffusing into the oil due to the concentration gradient) is mostly plausible because the injected CO
2 is not in direct contact with the resident hydrocarbon. On the other hand, Jia et al. [
1], based on the work of Habibi et al. [
15], depicted the recovery mechanism as follows: at low gas pressure (and at the interface of the fracture and matrix), the unidirectional diffusion of gas into the oil phase takes place, causing swelling and the expulsion of oil into the fracture; however, at a pressure above minimum miscibility pressure, two-way diffusion occurs and oil also diffuses into the gas in the fracture.
Some researchers have found that increasing the injection pressure results in higher recovery factors, leading to the conclusion that repressurization is the main recovery mechanism [
14]. Song and Yang [
21] showed that increasing the pressure only enhanced the recovery factor in the immiscible regime, while Adel et al. [
22] indicated that the recovery factor still increased with increasing pressure above the MMP.
Alfarge et al. [
23] reviewed and investigated the parameters affecting CO
2-EOR in shales using statistical methods. They found that the intensity of the fractures and the conductivity of the oil pathways were the two main factors affecting EOR efforts in shales. They argued that molecular diffusion is the main mechanism of recovery.
Field trials for EOR in shales are rare. Schmidt and Sekar [
24] reported the results of a pilot test in the Canadian Bakken in Saskatchewan. They used nine producer wells, which were 200 ft (61 m) away from the injection wells. Lean natural gas was injected at a rate of 350–1000 MScf/day (9.9–28.3 × 10
3 m
3/day) without any injectivity issues. The oil production increased in all nine producers; however, early breakthrough was observed in some of the wells. Todd and Evans [
25] reported the results of a pilot EOR test on US Bakken shale using CO
2 in different scenarios. Of the three CO
2 injections that were examined, two were performed in horizontal fractured wells using the huff-n-puff method. The other method injected CO
2 into a vertical well. The huff-n-puff tests showed no injectivity problems (1000 MScf/day (28.3 × 10
3 m
3/day) and 1500–2000 MScf/day (42.47–56.63 × 10
3 m
3/day) at 2000–3000 psi (138–207 bar)). However, no recovery improvements were observed. The third CO
2-EOR pilot injected CO
2 into the Middle Bakken Formation for 20–30 days, followed by 20 days of shut-in time while CO
2 breakthrough was observed in the offset wells that were 900 ft (275 m) away, after which the test was terminated. Another case tested the continuous injection of enriched natural gas into a well pattern of one injector and four producer wells. After injecting for 55 days at a surface pressure of 3500 psi (241 bar) and a rate of 1600 MScf/day (45.3 × 10
3 m
3/day), the production rate increased in the production wells. However, this could not be attributed to the injected gas as fracking hits from nearby wells could have interfered with the process. However, EOR activities in Eagle Ford shale have been successful at increasing production rates [
26].
Despite significant strides toward making CO2-EOR+ a reality in unconventional resources, there is still significant uncertainty surrounding the key design parameters that are necessary for successful EOR operation. Data from lab-scale tests and numerical simulations are promising, yet field-scale applications show missing links that need to be understood for the design of these recovery schemes. This, coupled with the movement toward net-zero and the large-scale deployment of CCUS projects, further necessitates investigation into the potential of CO2-EOR+ in unconventional reservoirs. The results from past studies have often been different and sometimes even contradictory. The recovery mechanisms are not well understood and the interactions between the CO2 and in situ hydrocarbons under nano-confinement is another area of active research. In this work, we performed a suite of characterization and CO2 extraction tests on four Canadian Bakken samples to understand the interplay of different properties within the recovery process. The pore and throat size, organic content, and in situ hydrocarbons were analyzed to better interpret the potential of CO2-EOR.
The methodology of the study is based on a comparative framework where CO2-EOR performance on four shale samples are compared. The characterization results were used for the interpretation of the CO2 extraction tests. This work is focused on the impact of shales’ properties on the EOR performance, rather than the operational parameters. It is important to note that this study focuses on the Bakken Formation, and consequently, it does not attempt to derive a correlation between shale properties and CO2-EOR performance.
4. Results and Discussion
The results section first presents the characterization tests followed by the CO2 extraction and recovery mechanism analysis. As mentioned earlier, the analysis is done in a comparative framework. Since the size of the sample set is small (four), the discussion is focused on interpreting the CO2 extraction results using the measured properties. However, since all four shale samples are from the same shale deposit, general correlations cannot be developed for predicting CO2-EOR performance (due to the limited variations in the properties).
4.1. Organic Matter Characterization and Thermal Maturity
The results of programmed pyrolysis of Lower and Upper Bakken samples with direct quantification of both TOC and TOS contents are presented in
Table 1. The amount of organic sulfur in sedimentary OM is a critical parameter that directly influences source-rock kinetics and, thus, thermal conversion of OM into hydrocarbons [
36,
37]. The samples are organic-rich with high TOC content ranging from 11.7 to 26.5 wt.% (
Table 1). The S1 and S2 values for all samples range from 4.6 to 10.6 and 68.4 to 154.4 (mg HC/g of rock), respectively. The hydrogen and oxygen indices (HI and OI) of all samples range from 562.3 to 627.8 (mg HC/g TOC) and 1 to 3 (mg CO
2/g TOC), respectively. The Tmax for all samples ranges from 431 to 435 °C along with a high HI value indicating the immature to marginally mature nature of samples (
Figure 2a).
The total sulfur (TS) content of the samples ranges from 1.5 to 6.3 wt.%, while TOS content ranges from 0.9 to 2.3 wt.% (
Table 1). Sulfide (i.e., pyrite) and sulfate are other major sulfur species in the samples and range from 0.5 to 3.4 wt.% and 0.1 to 0.7 wt.%, respectively (
Table 1). The sulfur index (SI) for all samples ranges from 23 to 30, which indicates a Type II marine kerogen (
Figure 2b) similar to Bakken Formation in the US (e.g., Carvajal-Ortiz et al. [
34]). Although the organic matter in the studied samples is marginally mature, the S1 peak is relatively high in all four samples, which means there is free oil in the samples to be recovered (
Table 1).
Organic petrographic observation and random bitumen reflectance (BRo) measurements of the samples further confirm the organic matter type (Type II) and low thermal maturity of the samples (
Figure 3;
Table 1). Both Upper and Lower Bakken samples from the studied wells are pyritic organic-rich shales with abundant solid bitumen and liptinitic alginite macerals (
Figure 3). The unicellular alginite (Prasinophyte) generally occurs in an amorphous bituminite kerogen network (
Figure 3) (e.g., Stasiuk [
38]). The alginite macerals in all samples exhibit green fluorescence, which indicates the low thermal maturity of the studied samples (
Figure 3b,d). There are two distinct populations of solid bitumen, one dominant with lower mean BRo ranging from 0.27 to 0.30% and a less abundant population with relatively higher BRo ranging from 0.46 to 0.51% (
Figure 3;
Table 1).
4.2. Pore Throat Size Distribution
MICP is a routine method for the determination of pore throat size distribution and porosity of porous sedimentary rocks. The technique is based on the Washburn equation and is limited to pore throats larger than 3.2 nm.
Figure 4 shows the cumulative and incremental pore volume obtained using the MICP technique. The cumulative pore volume plots reveal all four shale samples are broadly similar, with S1-UB having a slightly larger pore volume. Additionally, almost all pore volumes come from pores smaller than ≈100 nm.
The incremental pore throat volume plot (
Figure 4b) shows an exponential decay type profile, peaking at around 3–4 nm (the limit for the MICP method). All shale samples have similar pore throat sizes, with no indications of a noticeable peak.
The median pore (throat) diameter for all the samples is about 5.3–5.4 nm, while the average pore throat diameter is around 7.5 nm. This is typical of Canadian Bakken shale, which has a larger pore throat size compared to the US Bakken [
23]. The measured porosity (using the MICP method) is 3.7, 3.0, 3.2, and 3.7% in the order of presentation in
Figure 4.
The data from MICP analysis indicate largely similar samples in terms of pore throats size. There is no significant disparity either in the form of size or type of distribution in these samples. All four shale samples are ultra-tight.
4.3. Pore Throat Size Distribution
Pore size distribution in shales is often calculated via the adsorption–desorption phenomena of CO2 and N2. N2 is used for pores larger than 2 nm and up to ≈300 nm. N2 adsorption–desorption was used in this work to determine the pore size distribution of the samples. The free oil blocking the pores in the samples prevented measurement of N2 adsorption–desorption isotherms without treatment, thus the samples were cleaned using an organic solvent. Note that sample treatment was done only for pore size distribution measurement, and other tests used the samples in the as-received condition.
Figure 5a reports the N
2 adsorption–desorption isotherms for the studied samples. N
2 adsorption isotherms can be used to investigate meso and smaller macropores [
39]. The adsorbed amount for low pressures (≤0.05) is relatively small for all the samples, indicating a lack of small mesopores in these samples. Low Tmax and consequently the low maturity of the organic matter in these samples suggests a lack of development of organic matter-hosted pores which is reflected by the isotherm measurements. Sample S2-LB has the highest adsorption capacity, which is almost twice as high when compared to S1-UB.
The isotherms and hysteresis loops (difference between N
2 adsorption/desorption isotherms) cannot be simply attributed to a certain classification [
40]. A combination of type III and type IV appears to best describe the isotherms. The hysteresis loop is of H3 type, which is consistent with the type IV curve that suggests the occurrence of mesopores and the capillary condensation phenomena. Type IV isotherms are common for mesoporous materials (pore diameters between 2 and 50 nm) [
39]. The shape and type of isotherms suggest slit-shaped pores in these samples.
The specific surface area (SSA) of samples is shown in
Figure 5b. SSA is computed from the N
2 adsorption data using the BET method [
41]. As per the data, the samples have broadly similar SSA. Lower SSA than a typical mature shale agrees with the programmed pyrolysis data.
The Barrett, Joyner, and Halenda (BJH) method [
42] was used to compute the pore size distribution (PSD;
Figure 6a,b) of the samples from the adsorption branch of the N
2 isotherms. The PSD (
Figure 6a) plots show that three of the samples have a unimodal distribution, while S2-LB has two peaks. All samples have a peak around 60–70 nm. The peaks occur in the macro-sized pore range. Sample S1-UB also has a hint of a second peak near the 3 nm pore size.
Figure 6b depicts the cumulative pore volume, where S2-LB has the highest pore volume and S1-UB the lowest.
Overall, the pore size distribution analysis indicates that both LB samples have a larger pore volume and adsorption capacity compared to their UB counterpart. Sample S2-LB has a secondary peak for pore width <10 nm.
4.4. XRD Data
X-ray diffraction data are reported in
Figure 7a,b.
Figure 7a illustrates the bulk mineralogy of the samples and
Figure 7b shows the mineralogy of the clay-sized fractions. All four samples are carbonate lean with abundant quartz and mica (muscovite/illite). Minor amounts of K-feldspar and pyrite occur in all samples and minor to trace plagioclase feldspar, chlorite, kaolinite, siderite, hematite, and marcasite occur in the samples. In general, the LB samples have slightly higher clay contents with lower quartz.
The semi-quantitative mineralogy of the <2 μm fractions is given in
Figure 7b. The samples have abundant illite, subordinate quartz, minor K-feldspar and pyrite, and minor to trace calcite and dolomite. The samples do contain an amorphous component, estimated on average about 25%.
4.5. Molecular Analysis of Organic Extracts from the As-Received Rocks
The following section summarizes the distribution of organic compounds that were solvent-extracted from the samples. It should be emphasized that the molecular analyses of solvent extracts and the CO2 extracts (that will be presented later in this manuscript) are not comparable for two main reasons: (i) the solvent extracts have been fractionated into saturate and aromatic compounds whereas the CO2 extracts have been analyzed as whole oil, and (ii) the solvent extracts have been analyzed using GC-FID and GC-MS whereas the CO2 extracts were analyzed using GC-FID only, the latter limits the number of compounds that can be used for organic geochemical interpretations. However, the analysis of solvent extracts from as-received rocks was necessary to complement the general characteristics of the samples as well as examine possible relationships between their molecular nature and the petrophysical properties of the rock. In this section, only the findings on the organic compounds from rocks extracted with a solvent is discussed.
The relative distribution of n-alkane hydrocarbons contained in each sample is shown in
Figure 8. The samples exhibit a high abundance of light hydrocarbons in the C13–C16 range despite volatility loss during sample preparation. Hawthorne et al. [
7] showed, due to the tight nature of the shales, hydrocarbons tend to remain in the UB and LB rock samples much better than in the MB samples after collection and storage, though there are still losses of the more volatile hydrocarbons. A C13–C16 dominant composition for the in-place hydrocarbon is observed for all four shale samples. There is no significant disparity in the n-alkanes distribution (
Figure 8). Traces of heavier than C20 components are detected, particularly in sample S2-LB.
An important aspect to highlight is that the molecular data do not fully support the immaturity of the samples. For instance, the distribution of trimethylnaphthalenes (
Figure 9a) and tetramethylnaphthalenes (
Figure 9b) rather describes an early-mature to medium maturity as defined by van Aarssen et al. [
43]. Likewise, when correlating the trimethylnapthalene ratio (TMNr) with the tetramethylnapjthalene ratio (TeMNr) in
Figure 9c, these parameters do suggest a higher maturity level in the Lower Bakken (as expected for a normal maturity trend increasing with depth). In immature samples, the TMNr and TeMNr usually do not show any correlation due to stronger source effects that have not been overprinted by temperature [
43].
The alkylnaphtalene ratios are probably a better representation of the actual thermal maturity of the samples given the oil saturation found, which would not be expected for an immature rock. Previous studies have reported that highly organic-rich Bakken intervals tend to show underestimated maturity because of hydrocarbon carryover into the S2-pyrolysis peak, which leads to Tmax values lower than expected [
29,
44].
4.6. CO2 Extraction Data
As described earlier, CO2 extraction experiments measured both the cumulative and component-specific recovery factors throughout the tests. Cumulative recovery is simply the fraction of recovered hydrocarbon after each cycle of injection. Total recoverable hydrocarbon was computed by pulverizing the samples at the end of each test and extracting all hydrocarbons to compute the total hydrocarbon contents.
The cumulative recovery factors are reported in
Figure 10a. The recovery percentage at the end of the 24 h ranges from 42 to over 80%. Note that the recovery factors are high because the experiments were conducted on rock chips (due to increased surface area and pore accessibility). A notable feature of the recovery data is that the LB samples yielded higher recovery factors as compared to the UB samples. For sample S2, the recovery factor for the LB sample is almost twice that of the UB. The cause of such observation is not clear at first. Both sets of samples were analyzed for different characteristics, and LB samples tend to have higher pore volumes and are more mature than UB samples (see
Figure 5a and
Figure 9c).
Hawthorne et al. [
7] studied recovery from 51 US Bakken shale samples and observed that LB and UB samples are generally similar in their recovery factors. However, our dataset suggests the same might not be true for the Canadian Bakken Formation. To better understand the data, the recovery data should be combined with the other characterization tests. S1-UB has a higher TOC content than S1-LB, while S2-UB and S2-LB have relatively similar TOC contents. Therefore, TOC content is not the reason for recovery factor differences. On the other hand, LB samples tend to be more mature (see
Figure 9c) compared to UB samples. Higher maturity can potentially mean a better developed organic-pore system, that eventually affects the ultimate recovery factor.
It is also plausible that different depositional environments for the LB and UB layers could have an impact as well. For example, typical biomarkers such as hopanes and steranes were barely detected in sample S2-LB compared to the others, which might be attributed to depositional environment conditions. However, it is unclear how this would affect physical phenomena like CO
2 transport. Longer chain n-alkanes were also detected in sample S2-LB (
Figure 8).
In terms of pore structure, MICP data does not show significant differences in pore throat size between the LB and UB samples. However, the LPA data suggest that LB samples are more heterogeneous and have more mesopore volume, reflected through the hysteresis loop of the adsorption and desorption isotherms. The LB samples, in particular for sample S2, showed higher adsorption capacity (see
Figure 5a), and this may play a role in the differences in the recovery factors.
The mineralogy of both set of samples was also shown to be broadly similar, with the LB samples having slightly higher clay contents. In particular, higher illite contents may cause a reaction with CO
2 resulting in swelling of the clay contents [
45]. Clay swelling in an unconfined test can result in the development of micro-fractures in the samples, consequently improving contact area and permeability.
Combining the characterization results with that of CO2 extraction data, none of the properties can explain the differences between the recovery factor difference of LB and UB samples. If there is a correlation between these characteristics and the CO2-EOR performance, it is a highly complex and multi-dimensional relationship. Although there are differences in the adsorption capacity of samples, the CO2 extraction results do not correlate with the adsorption capacity (S1-UB has the lowest adsorption capacity, while S2-UB has the lowest recovery percentage). The difference in recovery factors of LB and UB samples can be explained partly by the maturity of the organic contents, where LB samples tend to be more mature. By extension, the difference might be attributed to better connectivity of the pores. Since the size of the dataset is limited in this work, no conclusion can be drawn on the role of mineralogy and wettability on EOR performance.
Figure 10b shows the incremental recovery factor recorded after each cycle of CO
2 injection and draw-down (at constant pressure). As expected, the first cycle has the highest recovery factor, and monotonic decrease thereafter until the 6th cycle. The last cycle is the longest in duration and the recovery factor increases compared to the previous cycle.
Comparing the LB and UB samples, the first cycle reveals a significant disparity. Both LB samples have almost identical recovery factors after the 1th cycle. The UB samples have almost half the recovery factor compared to the LB samples after the 1st cycle.
Figure 10b suggests CO
2 penetrates the LB samples much faster, possibly reflecting the difference in pore system structure of the LB and UB samples.
Hydrocarbon extracts during the CO
2 huff-n-puff experiments were also analyzed using GC–FID.
Figure 11 reports the component-specific recovery factors. The y-axis is the recovery factor for each component. The data suggest lighter hydrocarbons are easier to produce, and the ultimate recovery factor is higher for the lighter components. Higher solubility in CO
2, higher diffusion coefficient, and smaller molecular size are the main contributor to this behaviour [
17]. All samples show similar profiles. Note that the hydrocarbon composition for the samples indicates a light oil. The recovery data agrees with the diffusive recovery mechanism of Mahzari et al. [
18]. In essence, the concentration gradient drives the CO
2 into the oil, causing liberation of lighter components and consequently recovering hydrocarbons.
4.7. Recovery Mechanism
The recovery mechanism of oil through CO
2 huff-n-puff has been the subject of various studies. Most studies attributed EOR through CO
2 injection in shales to molecular diffusion of CO
2 into nano-pores (e.g., Alfarge et al. [
23]). The recovery factors profiles (
Figure 10a) are log-linear, which suggests a diffusion-dominated recovery mechanism. To test this hypothesis, the recovery profiles were fitted using a 1D concentration-gradient-driven diffusion type of recovery. Equation (
1) describes a recovery profile purely driven by diffusive flow [
16,
46]. Such assumption is based on the fact that the soaking chamber is static; it is further assumed that the pressure gradient tends to be negligible in the crushed samples. Once again, because of the small size of the particles (1–4 mm), such an assumption is justified. The recovery profiles are fitted to Equation (
1):
In Equation (
1),
X represents the length scale associated with the samples and D is the diffusion coefficient. The length scale implicitly includes the tortuosity of the pore space, which is an important factor in fluid flow and the accessibility of pores by CO
2. Since the length scale and the diffusion coefficient were unknown, they were combined into another parameter:
, which is the fitting parameter for the recovery data. The hypothesis is that when a fit to the recovery factor could be found using Equation (
1), the recovery was dominated by molecular diffusion, otherwise a more complex mechanism of recovery was at play.
Figure 12 shows the results of fitting Equation (
1) to the recovery profiles for the four shale samples. The recovery profiles for the LB samples (
Figure 12b,d) fit perfectly with a diffusion-driven type of recovery. UB samples (
Figure 12a,c), on the other hand, deviate from this behaviour. Sample S2-UB has the lowest recovery factor, and the recovery profile deviates from the concentration-gradient diffusion recovery profile.
A combination of various parameters appears to be causing a complex chain of reactions that ultimately results in the hindered ability of CO2 to diffuse into the tight shale matrix of the UB samples. However, based on the characterization results, this is not attributed to routine properties such as pore size distribution. Complex pore structures, low maturity, blocked pathways, and underdeveloped pore system in the UB samples are believed to be the main cause of deviation from a diffusive recovery. Parameters such as connectivity of the pore space, tortuosity, and diffusion coefficient play a crucial role in diffusion-driven flows. However, these parameters are not routine and are not measured in most studies.
It can be concluded that the main recovery mechanism of CO2-EOR in the experiments is molecular diffusion, driven by the concentration gradient. The design of EOR projects should take into account the importance of CO2 diffusion into the rock matrix to maximize oil recovery.
5. Summary
CO2-EOR+ in unconventional resources and, in particular, organic-rich shales has great potential, both financially and technically. However, field applications have seen limited success, with the exception of those at the Eagle Ford. Unlike conventional CO2-EOR, in which multiple drive mechanisms can contribute to oil recovery, concentration gradient-driven molecular diffusion is the primary mechanism of recovery in unconventional reservoirs. Field applications should be designed to maximize this diffusion. The fracturing, controlling flow conformance, soak times, and detailed characterization of the target formations would be key for these designs.
In this work, CO2-EOR performance in four Bakken shale samples was studied. The samples were characterized for pore and throat size, mineralogy, and geochemical property (organic petrography). These properties were used to analyze the CO2 extraction data. Since only four shale samples from the same shale deposit were used, the analysis was done in a comparative framework rather than isolating shale properties to study their impact on the CO2-EOR. We used the differences between the shale samples to explain the CO2 extraction data. However, it should be noted that no claim can be made about a single shale property on the CO2-EOR performance based on the results of this study. In the context of CO2-EOR and the impact of shale properties, most of these properties are confounder variables (i.e., they affect both the EOR performance and other properties). In presence of confounding variables establishing a clear correlation is not trivial and requires massive datasets to do.
In terms of factors affecting CO2-EOR in unconventional reservoirs, there is no clear indication of whether organic contents and mineralogy play a role. In the experiments conducted in this work with two sets of Lower and Upper Bakken shales, Lower Bakken samples have higher recovery factors compared to the Upper Bakken shales. The characterization tests indicated both formations are broadly similar in terms of pore structures, although the Upper Bakken samples tend to have higher TOC content. Nonetheless, both formations have very high TOC values, hence, it is hard to link the degradation in recovery factors to a single characteristic.
The analysis of the recovery mechanism shows that the maximum recovery factor is achieved under a concentration gradient driven diffusion drive mechanism. Of course, this is naturally the main mechanism of recovery since the test procedure constrained the convective transport (i.e., small to zero pressure gradient). However, the upper Bakken samples indicated a deviation from this regime, possibly owing to the pore structures and underdeveloped pore system that limits the fluid exchange. The deviation of recovery profiles from a concentration gradient driven diffusion dominant flow can potentially be caused by a combination of complex pore structures (e.g., large tortuosity) and immature organic contents of the samples.