The detailed characteristics of CNCs used in this study are summarized in Table 1, and their TEM micrographs are displayed in Figure 1. CNCs exhibited a short rod-like morphology with a width range of 5~20 nm and length of 50~100 nm. Its aspect ratio was approximately between 2.5~20. After the carboxylation treatment, negatively charged carboxy groups were introduced on the surface of CNCs, which contributed to the colloidal stability under the electrostatic repulsion. The ζ potential also proved this result. CNCs performed ζ potential values of -22.1 mV at pH 6.95 and -31.5 mV at pH 9.16. Figure 1b showed the apparent viscosity versus shear rate for CNC suspensions at concentrations of 0.5 and 1.0 wt %. All CNC suspensions exhibited low viscosity at high shear rates, but high viscosity at low shear rates, which was commonly called as “shear-thinning” behavior(Yang Gang 2021). Moreover, the shear-thinning phenomenon became more significant as the concentration of CNCs increased from 0.5–1.0%, which was desired performance of a drilling fluid. It can be inferred that CNCs can play a positive role on the rheological and filtration performance of BT-WBDFs.
Table 1
Physicochemical Characteristics of CNCs
sample
|
width (nm)
|
length (nm)
|
aspect ratio
|
ζ potential (mV)
|
pH
|
surface functional groups
|
CNCs
|
5~20
|
50~100
|
2.5~20
|
-22.1
|
6.95
|
-OH/ -COO−
|
BT-WBDFs are greatly expected to be typical shear-thinning non-Newtonian fluids, which have high viscosity at low shear rates to suspend or carry cuttings from downhole, but low viscosity at high shear rates to reduce friction and assist rock breaking(Fagundes et al. 2018). CNCs were incorporated with BT suspensions to explore how profitable CNCs modified the rheological properties of BT-WBDFs. The concentrations of CNCs were varied in the range of 0.25 to 1.0 wt %, while that of BT was fixed at 2.0 wt %. Figure 2a,b showed the plots of viscosity versus shear rate for BT/CNC suspensions at different CNC concentrations and temperatures. All samples revealed a shear-thinning behavior in the whole range of shear rates. But BT and BT/CNC suspensions presented distinctive shear-thinning behaviors after high temperature treatment. At room temperature, BT suspension exhibited a predictable shear-thinning property, thereby being commonly used in WBDFs(Farag et al. 2019, Zou et al. 2019). The addition of CNCs effectively increased the viscosity of BT suspension and produced more remarkable shear-thinning behavior, which was conducive to optimizing drilling fluid performance. For example, at the shear rate of 1.0 s−1, the addition of 0.25, 0.5, and 1.0 wt% CNCs into BT suspension increased the apparent viscosity values from 201.59554 to 740.77179, 1602.26233, and 4702.94775 mPa·s, respectively. In comparison with the result at room temperature, the high temperature processing at 140°C sharply decreased the viscosity of pure BT suspension, but the viscosity of BT/CNC suspensions maintained highly values, and the shear-thinning behavior was more outstanding. Moreover, it can been seen that the shear-thinning behavior for BT/CNC suspensions at room temperature was progressive, whereas that for BT/CNC suspensions at 140°C was nonprogressive, in which all BT/CNC suspensions displayed similar viscosity values at low shear rates, and progressive viscosity variation at high shear rates. For example, at a shear rate of 1.0 s−1, BT/CNC suspensions with 0.25, 0.5, and 1.0 wt % of CNCs had viscosity values of 2353.05176, 2851.86499, and 3578.5708 mPa·s, respectively, while at a shear rate of 119s−1, that were 21.98516, 48.28335, and 65.98486 mPa·s, respectively. Based on these observations, it can be concluded that CNCs can efficiently improve the shear- thinning properties of BT suspensions, even under high-temperature conditions.
Furtherly, the curves of shear stress versus shear rate for BT/CNC suspensions at different CNC concentrations were shown in Figure 2c,d. Similar to the viscosity results, the shear stress also enhanced with the increase in the concentration of CNCs. The Bingham plastic, power-law and Herschel−Bulkey models were applied to fit their shear stress−shear rate curves, and the corresponding fit parameters were listed in Table 2. Whether room temperature or 140°C, the Herschel−Bulkey model was more befitting for all shear stress−shear rate curves, compared with the Bingham plastic and power-law models, which was evidenced by the higher values of R2. In detail, after the addition of CNCs, the yield point values increased and the the flow behavior n index decreased with the increase of CNC concentration. The yield point indicated the stress required to start the flow of drilling fluid(Syed M. Hussaini 1983), which could reflect the strength of grid structure between clay particles and CNCs(Ismail et al. 2016). The rheological modeling results further proved that CNCs had superior rheological modification ability, beneficial for transporting the cuttings and cleaning the wellbore(Liu et al. 2017).
Table 2
Calculated Parameters for BT/CNC suspensions at different CNC concentrations using Bingham, Power-Law, and Herschel−Bulkley Models
models
|
parameters
|
CNC concentrations (wt %) / 25°C
|
CNC concentrations (wt %) / 140°C
|
0
|
0.25
|
0.5
|
1.0
|
0
|
0.25
|
0.5
|
1.0
|
Bingham
|
τ0
|
0.20732
|
1.22334
|
2.4135
|
6.04269
|
0.13684
|
1.69228
|
3.22997
|
5.91782
|
µp
|
0.00281
|
0.00692
|
0.0118
|
0.0226
|
0.00455
|
0.00595
|
0.01065
|
0.01377
|
R2
|
0.99703
|
0.97906
|
0.98173
|
0.98159
|
0.99744
|
0.97721
|
0.90405
|
0.99178
|
Power-Law
|
K
|
0.01714
|
0.21803
|
0.48434
|
1.54894
|
0.0118
|
0.46404
|
0.9233
|
2.30946
|
n
|
0.73984
|
0.50595
|
0.46988
|
0.40049
|
0.86143
|
0.38293
|
0.37155
|
0.28415
|
R2
|
0.9895
|
0.98066
|
0.97835
|
0.96581
|
0.99891
|
0.95897
|
0.97517
|
0.90854
|
Herschel−Bulkley
|
τy
|
0.16301
|
0.78231
|
1.65015
|
4.55636
|
0.05762
|
1.30569
|
1.10036
|
5.40477
|
K
|
0.00525
|
0.04815
|
0.0836
|
0.16378
|
0.00901
|
0.04256
|
0.45219
|
0.05044
|
n
|
0.90802
|
0.71707
|
0.71458
|
0.71131
|
0.8996
|
0.71313
|
0.46514
|
0.80994
|
R2
|
0.99862
|
0.9954
|
0.99928
|
0.99957
|
0.99942
|
0.99329
|
0.97909
|
0.99921
|
Based on above measurement results, it can be speculated that there must be particular surface interactions between CNCs and BT layers. To verify the interactions and driving force between CNCs and BT, the macroscopic phenomenon and microstructures of BT/CNC suspensions were examined, respectively. As displayed in Figure 3, pure BT suspension could easily flow after being placed for 10h, while BT/CNC suspension added with 1.0 wt% CNCs formed a whole piece of gel, indicating that BT/CNC had higher viscosity and stress. Moreover, after shaking for 10s, the formed BT/CNC gel could flow again. These distinctive phenomena between pure BT and BT/CNC suspensions demonstrated that CNCs had a strong gel formation capacity and a stiff network among BT layers, CNCs, and water molecules was created, which had a strong resistance to flow under shear force(Wang et al. 2018). The phase interactions between CNCs and BT layers were also observed by TEM (as shwon in Figure 4). BT hydrated in water and presented typical sheet-like structures (Figure 4a). In BT/CNC suspensions, CNCs were homogeneously dispersed in BT layers and they were entangled with each other (Figure 4b,c,d). The observations meant that CNCs were adsorbed onto the surface of BT particles and a stable colloidal structure was formed.
It was clear that BT was composed of a large number of plate-like crystal layers with permanent negative charges due to isomorphic substitutions on the faces and pH-dependent charges developed on the surface hydroxyls at the edges(Anderson 2010). Due to the broken bonds of the octahedral Al–OH and tetrahedral Si–OH groups on the edges, some amphoteric sites are also existing and variable (either positive or negative) charges can develop at the edges depending on the pH. Besides, a positive charged edge could be also created due to the exposed octahedral Al layers when the pH value is less than 9 (Tombácz 2006, Avena 2003). In pure BT suspension, the ionic attraction between the negatively chared face and positively charged edge (edge-to-face attraction) could form a “house-of-cards” structure, which was responsible for the viscosity of BT suspensions(Li et al. 2020). Therefore, BT was commonly used as a ideal additive in drilling fluid. In BT/CNC suspension, CNCs would adsorb to the surface of BT layers via hydrogen bond between their hydroxyl groups, and ionic bond between the positively charged edges of BT layers and the negatively charged carboxy groups of CNCs. Meanwhile, in addition to the hydration and colloidal properties of BT itself, CNCs also had strong gel formation capacity, due to the high specific surface area and a large number of hydroxyl groups on the nanoparticle surface(Robert J. Crawford 2012). Then a large number of water molecules were bounded at the vicinity of BT and CNCs and a compact network was created, leading to a strong resistance to flow under shear force, even at high temperatures. Based on above interaction, a significnt improvement in the rheological properties was achieved.
Filtration property is one of the most important properties for drilling fluids. The penetration of fluids into the formation always causes shale swelling and wellbore collapse. Furthermore, high temperatures may also destroy the hydration of clay and induce the flocculation of BT particles. Poor filter cakes with large thickness and high porosity formed on the wall of wellbore, resulting in large fluid loss volume and poor filtration property(Wang et al. 2021). As shown in Figure 5, the API fluid loss volumes of BT and BT/CNC suspensions were measured at different temperatures. After treatment at high temperature of 140°C, the fluid loss volume of pure 2.0 wt% BT suspension increased from 41.0 ml to 50.0 ml, revealing the detriment of high-temperature environments. By contrast, whether at room temperature or high temperatures, the addition of CNCs always improved the filtration performance of BT suspensions. The fluid loss volume of BT/CNC suspensions decreased as the concentration of CNCs increased, whereas the filter cakes also became thinner. No matter how CNCs worked, the filter cake was the final barrier to prevent filtration. It could be inferred that more suitable structure was formed in the filter cakes after adding CNCs as fluid loss reducer.
For drilling fluids, it is always thought that the filtration property is mainly determined by fluid viscosity and filter cake quality(S.M. Elkatatny 2011). Generally, high viscosity improves the fluid with the ability to against fluid loss(Borges et al. 2021). As analyzed in Figure 2a,b, the viscosity increased with increaseing the concentration of CNCs. However, the viscosity of BT/CNC suspensions at low shear rates under 140°C processing varied mildly, which was mainly related to the API fluid loss volume under static filtration condition. Therefore, increasing viscosity might be not the predominant factor affecting the filtration control property of CNCs. Then, the microstructure of filter cakes was further detected by SEM observation (as shown in Figure 6). At room temperature, it could be seen that both of the BT and BT/CNC presented satisfactory filter cakes with smooth and hydrated surface. Furthermore, the filter cakes obtained from BT/CNC suspensions exhibited more pronounced “colloid texture”, like a polymer film. Similar phenomena also went for high tenperature environment of 140°C. In order to observe the deposit structure of BT layers more clearly, the cross sections of these filter cakes were also investigated, as displayed in Figure 7. Obviously, the sections from BT/CNC were more regular and compact than that from pure BT, especially at high temperature. BT layers in BT/CNC deposited regularly under differential pressure and formed a clear lamellar structure, which was beneficial for producing thin and compact filter cakes.
Interestingly, we also found that the addition of CNCs improved the hydrophobicity of the filter cakes. As exhibited in Figure 8, filter cakes from pure BT displayed strong hydrophilcity and had a water contact angle of approximate 27 ° at room temperature and 140°C. Adding CNCs dramatically enhanced the water contact angle of the filter cakes. For example, at a CNC concentration of 1.0 wt %, the water contact angle of the filter cake obtained from BT/CNC suspensions was increased to 57.78 and 66.67 ° at room temperature and 140°C, respectively. The enhanced hydrophobic effect was favorable for preventing the invasion of water(Saparti et al. 2018). Besides, according to Wenzel’s equation(Wang et al. 2015), the decrease of roughness can increase the contact angle measured on hydrophilic surface. The contact angle measurement also proved that the the addition of CNCs caused a more smooth surface on the filter cakes.
In short, based on the gel network among BT layers, CNCs, and immobilized water molecules, and the adsorption of CNCs on BT surface, BT deposited on the filter paper in a regular and compact layered structure, forming a more hydrophobic and smooth CNC polymer film on the surface. Finally, a high-quality filter cake was built and the fluid loss volume was sharply decreased.
In comparison with OBDFs, one of the deficiencies of WBDFs is the insufficient inhibition. There are more water in WBDFs and the fluids easily penetrate into the formation, resulting in clay hydration, swelling, and dispersion. Therefore, efficient shale inhibitors must be added in WBDFs (Muhammed, Olayiwola and Elkatatny 2021). The inhibition of CNCs was evaluated by linear swelling measurement and shale recovery test. As shown in Figure 9a, the swelling height curves of all samples exhibited a similar tendency with a dramatic increase rate within the initial period and a gradual slower growth as time proceeds, which was the typical swelling behavior of BT in aqueous solution. However, there was a gradual decrease in swelling height after CNCs were added as inhibitors. In detail, after immersing in water for 24 h, the swelling height of BT pellet in pure water reached as high as 6.16 mm. In comparison, the linear swelling heights of the BT pellets in filtrate obtained from BT/CNC suspensions at a CNC concentration of 0.25, 0.5, and 2.0 wt % CNCs were 5.77, 5.23, and 4.00 mm, respectively, displaying the inhibition property on BT swelling. Shale recovery test, as a standard method for evaluating the hydration dispersion of shale cuttings after hot-rolling at a set temperature, was also conducted. As illustrated in Figure 9b, after aging at 140°C, the shale recovery value of pure BT suspension was the lowest (29.4%), which indicated the strong water sensitivity and dispersion of shales. Under the same conditions, the shale recovery values for BT/CNC suspensions with 0.25, 0.5, and 1.0 wt % of CNCs were 35.8, 48.6, and 55.25%, respectively, suggesting the capability of CNCs for inhibiting the dispersion of the shales. Moreover, the results from hot-rolling shale recovery tests also demonstrated the temperature resistance of CNCs. The findings from linear swelling tests and shale recovery experiments were consistent. CNCs could used as valid inhibitors in WBDFs.
Generally, shale inhibitors achieved efficient inhibition through decreasing the interlayer spacing, such as KCl, the oligomeric and polymeric amines with cationic groups(Anderson 2010), or encapsulation effect, such as various acrylamide copolymers(Zhang et al. 2018). Visibly, CNCs, as negatively charged solid-phase nanoparticles, might not inhibit BT by these approaches, presumably due to the interactions (gel network and adsorption) between CNCs and BT particles analyzed above, or whether there were other mechanisms. With these questions, the colloidal stability of BT was examined by measuring the ζ potential and particle size distribution. As shown in Figure 10, the addition of CNCs decreased the ζ potential efficiently. When the concentration of CNCs was 1.0 wt %, the ζ potential of BT decreased from -23.05 mV to -32.4 mV at room temperature. The variation tendency of the ζ potential at 140°C was similar with that at room temperature. However, the whole values of the ζ potential at 140°C were higher, echoing the increase of fluid loss volume from 25 to 140°C in Figure 5. Anyway, the cooperation of CNCs could increase the negative charges of BT particles and improve their stability.
Meanwhile, the particle size distribution of BT/CNC was also determined. As exhibited in Figure 11, the addition of CNCs didn’t increase the particle size of BT, even showing a dispersion effect at small size range. These results demonstrated that CNCs didn’t inhibit the hydration and swelling of BT by encapsulating the BT particles.
The ζ potential and particle size measurements indicated that CNCs could promote the stability of BT suspensions, which was contrary to the general inhibition mechanisms mentioned above. How does CNCs exert competent inhibition? In order to figure this out, the water activity of these samples were further evaluated (as listed in Table 3). Water activity is an important index in estimating shale/drilling fluid interactions, which can evaluate the hydration state of shale and its potential to adsorb or lose water. Drilling fluids with lower water activity than shale can reduce the osmotic pressure between drilling fluids and the formation fluids, finally preventing water from invading shales(Chenevert 1970, Jianguo Zhang 2008). From the Table 3, the water activity of BT samples decreased gradually with increasing the concentration of CNCs from 0 to 1.0 %. In fact, these results should be foreseeable. The rheological tests concluded that BT, CNCs and immobilized water molecules formed stiff gel network. This network could efficiently bound the water molecules and reduce the free water, thereby decreasing the water activity. Moreover, the filtration measurements indicated that CNCs could contribute to creating a thin, compact, and low-hydrophilicity filter cake. The plugging and wettability modification abilities of CNCs aslo restrained the penetration of free water into the clay or shales. Under these comprehensive actions, CNCs presented the inhibition well.
Table 3
The water activity of BT/CNC suspensions at different CNC concentrations after aging at 25°C and 140°C.
sample
|
water activity /aw
|
25°C
|
140°C
|
BT
|
0.968
|
0.964
|
BT+ 0.25% CNCs
|
0.953
|
0.954
|
BT+ 0.5% CNCs
|
0.933
|
0.932
|
BT+ 1.0% CNCs
|
0.927
|
0.931
|
In summary, the modification effect of CNCs on the properties of BT-WBDFs and the interaction mechanism were concluded and listed in Table 4, which was also clearly described by the schematic diagrams, as shown in Figure 12. BT platelet was negatively charged on the flat surface and positively charged on the edge. These plates could be linked together via face-to-face (FF), edge-to-edge (EE), and edge-to-face (EF) attractions. The edge-to-face attraction formed a “house-of-cards” structure, which was responsible for the viscosity of BT suspensions. When the CNCs were employed in BT suspensions, one hand, CNCs adsorbed on the surface of BT through hydrogen bond and electrostatic interaction. The BT platelet and CNCs interwove with each other and formed stable “house of cards” structure at low shear rates and dispersed structure at high shear rates. On the other hand, due to the strong gel formation capacity of CNCs, a stiff network between BT layer, CNCs, and water molecules was created. Finally, BT/CNC suspensions exhibited excellent “shear- thinning” property. Based on the prominent rheological properties and plugging function of CNCs, BT/CNC deposited on the filter paper with a compact layered structure and constituted a “film” with improved hydrophobic ability, thereby resulting in a thin and compact filter cake and low filtration volume. Meanwhile, under the actions of CNCs, BT/CNC suspensions kept colloidal stability with high viscosity, displayed lower water activity, and prevented the penetration of free water, exerting competent inhibition on hydration and dispersion of clays. As a result, CNCs performed great potential to be used as efficient and environmental-friendly rheological modifier, fluid loss agent, and clay inhibitor for BT-WBDFs.
Table 4
The functions and mechanisms of CNCs on improving the peoperties of BT-WBDFs
|
Effect
|
Mechanism
|
Rheological property
|
The addition of 1.0 wt % CNCs increased the yield point of BT suspension from 0.13684to 5.91782 Pa at 140°C.
|
Adsorption of CNCs on BT;
Stiff network between BT layer, CNCs, and water molecules.
|
Filtration property
|
The addition of 1.0 wt % CNCs decreased the API fluid loss volume of BT suspension from 50.0to 16.0 ml at 140°C.
|
Thin and compact filter cakes with layered structure;
Improve the hydrophobic property of filter cakes;
Plugging effect of CNCs.
|
Inhibition property
|
The addition of 1.0 wt % CNCs decreased the swelling height of BT in filtrate from 6.16 to 4.00 mm at room temperature. The addition of 1.0 wt % CNCs increased the shale recovery of BT suspension from 29.40 to 55.25 % at 140°C.
|
Adsorption of CNCs on BT;
Stiff network between BT layer, CNCs, and water molecules;
Low water activity;
Plugging effect.
|