Qiang Lia,
Yanling Wang*a,
Qingchao Lia,
Gomado Fostera and
Chuang Leib
aCollege of Petroleum Engineering, China University of Petroleum (East China), Qingdao, 266580, China. E-mail: wangyl@upc.edu.cn
bPetroChina Huabei Oilfield Company, Renqiu 062500, China
First published on 26th February 2018
Silicone polymer shows high performance for thickening supercritical carbon dioxide and has become a well-known target because it is inexpensive and environmentally friendly. In this study, siloxane polymer was synthesized by a copolymerization reaction. The synthesis conditions of the silicone polymer were optimized using a Box–Behnken design, and the yield from the process was considered as an evaluation criterion in the screening of the synthesis process. The thickening effect of the polymer was evaluated using an in-house-built ball viscometer with operation pressure not exceeding 30 MPa. The experiments clearly showed that temperature is the most crucial factor for the synthesis process. At higher preparation temperatures (>90 °C), the yield significantly decreased from the process. The stability of the yield was influenced by the change in the molar ratio and amount of the catalyst used in the preparation. The most optimal preparation parameter for the synthesis was at a temperature of 90 °C, with an aminopropyltriethoxysilane-to-methyl triethoxysilane molar ratio of 2:1, and 0.09 g of tetramethylammonium hydroxide as a catalyst. The test yield (84.51%) coordinated well with the predicted yield of 83.72%. Adding 3 wt% siloxane to pure carbon dioxide thickened it 5.7 times at 35 °C and 12 MPa. An enhanced yield trend was observed with increasing pressure and a temperature range of 35–55 °C. The application of CO2 fracturing technology can help to reduce the greenhouse effect and the environmental pollution caused by fluoropolymers as thickeners when silicone polymer is deployed as a thickener for CO2.
Currently, fluoropolymers have been recognized and deployed as good alternatives due to their enhanced solubility in CO2, and they have been applied in a wide range of CO2 fracturing projects in various oilfields.37–41 Despite their enhanced solubility, the application of fluoropolymers is limited because they tend to pollute the groundwater during the oilfield development process and they are very expensive when deployed as a thickener. Because of this, much research has been carried out to improve the performance of siloxane polymer with the assistance of a cosolvent.15,16 Because the performance of siloxane polymers is limited by their low degree of thickening, a large amount of cosolvent is required to achieve a higher viscosity necessary for thickening supercritical CO2. In view of the above limitation, reducing the amount of cosolvent and improving the thickening ability has become a challenge. From previous studies performed on siloxane polymers, it is believed that the molecule of siloxane polymer, which thickens supercritical CO2, should contain CO2-philic groups and CO2-phobic groups in appropriate proportions. More specifically, the main chain of siloxane polymer is a CO2-philic chain, and CO2-phobic groups should be linked to the side chain of the siloxane polymer molecule through other chemical reactions.12
In this study, we present the optimization of the synthetic process for silicone copolymer production using the response surface method (RSM). The structure of the molecule was inferred by Fourier transform infrared (FTIR) spectroscopy, and the thickening ability was measured using a custom-designed falling ball viscometer. The response surface method is used to obtain the optimum operating condition and the most significant interaction parameter among synthetic influencing factors.17,18 Our initial attempts in this study mainly focused on synthesizing a new thickener that can easily dissolve in supercritical CO2 using toluene as a co-solvent to induce a viscosity increase. A mathematical regression model of the Box–Behnken design was developed to obtain the best reaction conditions and evaluate the interaction among crucial preparation conditions, and the optimum technological condition was verified via relevant experiments. A higher yield of the product exists under these synthetic optimal reaction condition. For the viscosity testing, we designed a falling-ball viscometer that could measure the relative viscosity of a mixture of thickener and CO2. Finally, we report the trend of the viscosity with the change in the pressure and temperature.
The obtained yields were calculated according to eqn (1):
(1) |
(2) |
Factors | Symbol | Levels | ||
---|---|---|---|---|
−1 | 0 | +1 | ||
The amount of catalyst/g | X3 | 0.06 | 0.09 | 0.12 |
Molar ratio | X2 | 1.5:1 | 2:1 | 2.5:1 |
Temperature/°C | X1 | 80 | 90 | 100 |
Run | Temperature/°C | Molar ratio | The amount of catalyst/g | Yield/% |
---|---|---|---|---|
1 | 0 | 1 | 1 | 76.43 |
2 | 0 | −1 | 1 | 75.17 |
3 | 0 | 0 | 0 | 84.01 |
4 | 1 | 1 | 0 | 80.37 |
5 | −1 | 0 | 1 | 76.94 |
6 | −1 | −1 | 0 | 80.31 |
7 | 0 | 0 | 0 | 82.13 |
8 | 0 | 0 | 0 | 84.51 |
9 | 1 | 0 | 1 | 77.01 |
10 | 1 | −1 | 0 | 82.76 |
11 | 0 | 0 | 0 | 84.25 |
12 | 1 | 0 | −1 | 74.48 |
13 | −1 | 1 | 0 | 80.32 |
14 | 0 | 0 | 0 | 83.71 |
15 | −1 | 0 | −1 | 77.18 |
16 | 0 | −1 | −1 | 77.72 |
17 | 0 | 1 | −1 | 76.96 |
Y (%) = 83.72 − 9.5 × 10−3 × A − 0.24 × B − 0.09 × C − 0.60 × A × B + 0.71 × A × C + 0.51 × B × C − 1.47 × A2 − 1.31 × B2 − 5.84 × C2 | (3) |
The data summarized in Table 3 show the analytic evaluations of ANOVA, which fit the second-order response surface model for the yield of the silicone ternary copolymer. The variable is more significant due to the lower P-value, and the mathematical model is considered significant when the P-value is below 0.05.19,22 The high significance level of the fitted model is indicated by the F-value of 11.83 and the probability value less than 0.05 in Table 3. The occurrence of the probability of the model F-value of 11.83 because of noise is below 0.05. Also, the lack-of-fit F-value of 3.01 indicates that it is somehow not significant compared to the pure error. The P-value of 0.1577 implied that the model and the data are consistent. Additionally, R2 was used to evaluate the satisfaction capacity of the model, and in this case, the R2 value of 0.9383 reveals a small deviation between the actual values and the predicted values. In addition, a high range of the ability and an appropriate goodness-of-fit for the second-order response surface model is conveyed by the correction coefficient of determination (RAdj2 = 0.8590).25 For the value of RPred2 (0.2867), the same conclusion can be made for the adjusted determination coefficient. In addition, a good significant and negligible error is shown by the high value of the predicted determination coefficient. The precision, reliability, and repeatability of the yield of the product are indicated by a small coefficient of variation (CV% = 1.61), and the lower the value, the higher the precision, reliability, and repeatability.26
Source | Sum of squares | DF | Mean square | F-value | P-value, prob < F |
---|---|---|---|---|---|
Model | 174.42 | 9 | 19.38 | 11.83 | 0.0018 |
A | 7.22 × 10−4 | 1 | 7.22 × 10−4 | 4.41 × 10−4 | 0.9838 |
B | 0.44 | 1 | 0.44 | 0.27 | 0.6188 |
C | 0.068 | 1 | 0.068 | 0.042 | 0.8438 |
AB | 1.44 | 1 | 1.44 | 0.88 | 0.3789 |
AC | 1.99 | 1 | 1.99 | 1.21 | 0.3070 |
BC | 1.02 | 1 | 1.02 | 0.62 | 0.4559 |
A2 | 9.09 | 1 | 9.09 | 5.55 | 0.0507 |
B2 | 7.27 | 1 | 7.27 | 4.44 | 0.0731 |
C2 | 143.60 | 1 | 143.60 | 87.67 | <0.0001* |
Residual | 11.47 | 7 | 1.64 | ||
Lack of fit | 7.94 | 3 | 2.65 | 3.01 | 0.1577 |
Pure error | 3.52 | 4 | 0.88 | ||
Cor total | 185.89 | 16 |
As shown in Table 3, terms are indicated as significant if the P-value is below 0.0001.23,24 C2 is considered as significant by ANOVA because of the smaller P-value in Table 3. The P-value of C has an adequate influence on the yield of the product because the P-value is less than 0.0001. On the contrary, the numerical value shows that A, B, C, AB, AC, BC, A2, and B2 have no significant effect. These terms could be deleted and a modified model of this synthetic process could be generated.
The reason for the workings of the above model is summarized as follows. A large amount of energy was absorbed when the bond between the Si atom attacked by the catalyst and the O atom adjacent to this Si broke, and the bond of Si–O was easy to break with increasing reaction temperature (80–100 °C). Moreover, as an endothermic reaction, the hydrolysis reaction of methyl triethoxysilane and aminopropyltriethoxysilane requires the absorption of a great deal of energy, and the above three reactions showed a more sufficient reaction efficiency and a higher yield with the rise in temperature. Additionally, the molar ratio of methyl triethoxysilane and aminopropyltriethoxysilane and the amount of catalyst exhibited a smaller effect on the yield of the product. For the molar ratio, a decreased addition of methyl triethoxysilane and aminopropyltriethoxysilane were insignificant factors. For the amount of catalyst, the increase in yield of synthetic polymer was very small when the catalyst reached a certain amount. The catalyst affects only the reaction rate of the polymerization reaction, and there was a larger collision probability between the catalyst molecule and the octamethylcyclotetrasiloxane molecule to cause the shorter reaction time, but the smaller change for the yield of product is shown in this study.
The residuals could be used to evaluate the adequacy of the model and the normality assumption. The normal probability plot of the residuals is shown in Fig. 4a. The data points were uniformly distributed around a straight line, which was similar to the plots of normal probability versus the standardized residual. Based on this line, the independence of the residuals was clearly confirmed. As illustrated in Fig. 4b, it is observed that there are similar trends of the plot of the actual versus predicted values being close to a straight line. The model was considered accurate according to the diagonal line along which these points cluster in Fig. 4.
Fig. 4 The adequacy and the normality assumption of the model. The color change from blue to red represents a gradual increase in the yield of the product. |
Fig. 5 Line chart of a single factor with the yield. (a) Temperature, (b) molar ratio, and (c) the amount of catalyst. |
The influence of the interaction of temperature and catalyst upon the yield of the silicone ternary copolymer was determined using the three-dimensional response surface and two-dimensional contour plots, as shown in Fig. 6a. The molar ratio of 2:1 and reaction time of 5 h are seen as the central point, and it was also considered that the reaction of two factors was prominent because of the steep contour (line). The yield of the silicone ternary copolymer was observed to increase with increasing reaction temperature (80–90 °C). The highest yield of 83.02% was obtained at 90 °C. However, with higher temperatures (>90 °C), there was a decreasing trend of the yield. This occurred because the hydrolysis reaction was obstructed due to the high temperature. The yield also decreased with increasing temperature due to the volatilization of methyl triethoxysilane, aminopropyltriethoxysilane, and water. The yield did not change based on the amount of catalyst in the range of 0.06 g to 0.12 g, and sufficient catalyst was the primary reason.
Fig. 6b describes the effect of temperature as well as the molar ratio and the interaction of the above two factors on the yield value, and the amount of catalyst of 0.09 g was a prerequisite. The same regular pattern is presented in Fig. 6b that is comparable with Fig. 6a. More specifically, the change in temperature presents a greater influence on the yield than the molar ratio of the reagents.
Based on Fig. 6c, the interaction of the weight of the catalyst and the molar ratio was more insignificant compared with the other two interactions that are shown in Fig. 6a and b, and the central point was defined as the reaction temperature of 90 °C at a constant time of 5 h. Fig. 6c depicts a maximum value of the yield of silicone ternary copolymer at a temperature of 90 °C, a catalyst amount of 0.1 g, and a molar ratio of 2:1. The stable value of the yield of the product was found to be suitable for the range of the catalyst levels (0.06–0.12 g) and the molar ratio (1.5:1–2.5:1). More specifically, the temperature was the predominant factor that increased the yield, and the catalyst and molar ratio were in a reasonable range at this time.
Fig. 6a–c shows the interaction of temperature with the reactant ratio and the interaction of temperature with a catalyst for the yield of copolymer, and a significant influence is clearly presented. On the contrary, the smallest factor is shown by the interaction between the molar ratio and the catalyst. Overall, the greatest effect on polymer yield among the three factors investigated was caused by temperature.
A schematic showing the viscosity calculation for the silicone thickener is presented in Fig. 3. For a falling ball viscometer, accurate viscosity could not be obtained for the silicone thickener, but the multiples of viscosity between the mixture (silicone thickener and CO2) and pure CO2 were calculated precisely as shown in eqn (4), and it was designated as the relative viscosity. Compared with the capillary viscometer, the position of the steel ball at a specific time in the fluid was captured, and the average speed (v1 or v2) was solved according to the time difference (t1 or t2) and distance (l1 or l2). Obviously, the steel ball should maintain a state of equal velocity motion in the liquid, and the speed required (v1 or v2) should be considered as the average value of the velocity of three different distances in the uniform motion stage:
(4) |
Measurement equipment was custom-designed based on Stoke's law,27 and eqn (4) provides an analytical expression for the viscosity. In the state of uniform motion, Stoke's law and eqn (4) are applied. The two forces denoted as eqn (5) and (6) are always present during the descent of the ball.28
mg = V0ρsg = G | (5) |
(6) |
F = V0ρ0g | (7) |
The steel ball presents the state of force balance when moving at a constant speed. Hence, equating these three (eqn (5)–(7)), the force on the ball can be described as follows:
mg − Fr − F = 0 | (8) |
(9) |
(10) |
(11) |
(12) |
(13) |
As a supercritical fluid, Re = 23.03 was measured for CO2. Similarly, Re = 0.43 was obtained when 6.4 wt% siloxane was added to pure CO2. Eqn (11), which was used for Re in the range of 0.1 to 103, satisfied the requirement at the range of 0.43 to 24. Supercritical CO2 showed a laminar state due to the Re. Moreover, there was almost no change in the density of the fluid after a small amount of thickener and co-solvent were added.14 The laminar state still existed according to Re = 0.43. The relative viscosity between the mixture fluid and pure CO2 could simultaneously be considered as eqn (14).
(14) |
Compared with other measurement equipment, an accurate viscosity could not be obtained according to eqn (14), and the simplicity of the viscosity calculations is shown.
Polymer (wt%) | Cosolvent (wt%) | Temp (°C) | Pressure (MPa) | Relative viscosity |
---|---|---|---|---|
1 | 7 | 35 | 8 | 1.8 |
1 | 7 | 45 | 8 | 1.4 |
1 | 7 | 55 | 8 | 1.2 |
1 | 7 | 35 | 10 | 2.3 |
1 | 7 | 45 | 10 | 1.8 |
1 | 7 | 55 | 10 | 1.7 |
1 | 7 | 35 | 12 | 2.4 |
1 | 7 | 45 | 12 | 2.3 |
1 | 7 | 55 | 12 | 1.8 |
3 | 7 | 35 | 8 | 5.1 |
3 | 7 | 45 | 8 | 4.6 |
3 | 7 | 55 | 8 | 4.1 |
3 | 7 | 35 | 10 | 5.5 |
3 | 7 | 45 | 10 | 4.8 |
3 | 7 | 55 | 10 | 4.1 |
3 | 7 | 35 | 12 | 5.7 |
3 | 7 | 45 | 12 | 4.9 |
3 | 7 | 55 | 12 | 4.2 |
The thickening properties were the result of the combination of the following groups. As an electronic group, the NH2 in siloxane interacted with the CO2. More specifically, the lone pair of N that interacts with C lacked electrons in CO2, and CO2 was above the N.34–36 The OH in siloxane played a role in increasing the space grid structure formed by the polymer and CO2 molecules. In addition, the O of CO2 interacted with the C–H of the methyl group in toluene. Similarly, the C–H⋯O bond43–45 between the O of the siloxane backbone and the C–H of the methyl group in toluene explained the increased CO2 viscosity of the silicone-containing polymer. The thickening mechanism is shown in Fig. 8. A suitable ratio of CO2-phobic segments not only affected the solubility with the assistance of toluene but also improved the thickening performance.42 More specifically, a certain number of OH moieties improved the space grid structure to thicken the CO2. Nonetheless, the small intermolecular forces that result from big chain flexibility are the important factors that thickened the CO2.
The measurement equipment included a custom-designed falling-ball viscometer that was utilized to measure the thickening properties. The results showed that the relative viscosity of CO2 increased 5.7 fold upon addition of the mixed silicone copolymer fluid, which was inexpensive and more environmentally friendly than the polymers that have been described in previously published studies.
Water resources can be effectively protected by using a silicone polymer rather than a fluoropolymer. More importantly, CO2 fracturing technology could actualize the storage of CO2 to significantly ameliorate the greenhouse effect.
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