Open Access Article
Maryam Mokhtarifarab,
Jonathan Gauvin-Audetb,
Aliakbar Sarbanhac,
Reyhaneh Kavehd,
Jesse Greener
be,
Faiçal Larachi
*c and
Frédéric-Georges Fontaine
*b
aDepartment of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA
bDepartment of Chemistry, Université Laval, Québec City, QC G1V 0A6, Canada. E-mail: Frederic.Fontaine@chm.ulaval.ca
cDepartment of Chemical Engineering, Laval University, 1065, Avenue de la Medecine, Quebec G1V 0A6, Canada. E-mail: Faical.Larachi@gch.ulaval.ca
dDepartment of Inorganic Chemistry, Faculty of Chemistry, Kharazmi University, Tehran 15719-14911, Iran
eCHU de Québec, Centre de recherche du CHU de Québec, Université Laval, Québec, QC G1L 3L5, Canada
First published on 16th June 2026
Conversion of carbon dioxide (CO2) to cyclic carbonates is important for carbon capture and utilization and enables the production of valuable, non-toxic chemicals from a climate-relevant greenhouse gas. This paper reports a catalytic strategy for synthesizing cyclic carbonates using commercial solid mesoporous silica supports with controlled particle sizes. Tripropylammonium groups were grafted onto the silica surface to activate it for CO2 conversion. Batch reactor experiments confirmed that the functionalized silica catalyzes the reaction under milder temperature and pressure conditions than previously reported. Importantly, this strategy effectively suppresses polymer by-product formation, enabling selective cyclic carbonate production while offering potential applications for controlled polymer synthesis through reverse optimization. A subsequent gas-phase cycloaddition reaction was conducted in a micropacked bed reactor. The reactor performance was assessed using the chemical regime method to separate intrinsic kinetics from mass transfer effects. Compared to conventional fixed-bed reactors, the reaction times were significantly reduced, from several days in batch systems to ∼1 minute in centimetric reactors and <1 second in microreactors. These findings support the potential for commercial-scale implementation.
Inspired by Werner et al.,30 we reported that ordered silica mesoporous materials containing grafted ammonium moieties were efficient catalysts for the formation of cyclic carbonates from CO2 at ambient pressure.31 The high catalytic activity value of these heterogeneous materials, far beyond what Henry's law predicts, was attributed to the oversolubility of CO2 within the nanometric pores of the material.32,33 Indeed, a 7.5-fold rate enhancement of the catalytic activity was observed in grafted MCM-41, as compared to homogeneous catalysis in bulk solution under similar conditions.34 Monte Carlo simulations revealed that this improvement was due to a lower density of the absorbed solvent in the nanopore, a phenomenon that is optimal with a pore size of approximately 4 to 6 nm.34
Although ordered mesoporous silicas such as MCM-41 and SBA-15 exhibit high surface area, often close to 1000 m2 g−1, they are expensive to produce compared to irregular silica. If the hypothesis is correct that the enhanced catalytic activity observed for the formation of cyclic carbonate using epoxides and CO2 is caused by the nanoporosity of the catalytic support, commercial silica materials with pores in the optimal range of 4 to 6 nm should also exhibit enhanced catalytic activity. For validation, we investigated the catalytic activity of commercial irregular silica materials SiliaFlash Silica Gel, both in batch and flow processes, as reported herein.
The industrial relevance of the present results lies in process intensification rather than direct geometric scale-up of a single microreactor. Micro-packed beds are attractive because their small characteristic dimensions enhance heat and mass transfer and may allow access to reaction conditions that are closer to intrinsic kinetic behaviour than in larger reactors.35 In practice, translation to larger throughput would more realistically proceed through numbering-up of multiple micro-packed-bed channels operated in parallel, rather than by increasing the diameter of a single reactor and sacrificing the transport advantages of miniaturization. This perspective is also consistent with earlier analyses from our research group emphasizing that micro-packed-bed performance results from confinement-enhanced transport and hydrodynamics, but that practical implementation must still address pressure-drop management, flow distribution, and operability.35,36 In addition, we conducted a performance assessment of the micropacked bed reactor, which encompassed parameters such as catalyst dilution, reactor temperature, operating pressure, residence time, and the molar ratio of carbon dioxide to propylene oxide. The limitations of fluid–solid mass transfer were studied by extensively comparing the performance of the microreactor to that of conventional centimetric fixed beds. This comparative analysis serves as a preliminary step towards extrapolating the findings to commercial-scale units.
Overall, this study demonstrates that confinement-enhanced CO2/epoxide coupling with supported ammonium sites is achievable on inexpensive commercial silica gels and quantifies, via micro- versus centimetric-scale packed-bed benchmarking, the reactor-transport contribution to the observed flow performance.
:
1 ether/hexane mixture (Fig. S1 and S2 in the SI).
![]() | ||
| Fig. 1 Synthetic routes for (a) TPA, (b) grafting of TPA catalyst onto silica, and (c) TMDS passivation of TPA-grafted silica material. | ||
Tables S1–S5 and Fig. S3–S7 (in the SI, section S3) compare the contractions in pore diameter after grafting to the non-functionalized material, confirming the success of the procedure. The quantitative differences observed between the two functionalized catalysts, R170-TPA and R150-TPA, can be attributed to the higher amount of quaternary ammonium species grafted onto the surface of R170. Grafting success was also confirmed by thermogravimetric analysis during air burn-off of the grafted organic materials (SI, Fig. S9–S13, section S4). Fig. S14 shows the FTIR spectra after the grafting and passivation steps, thus confirming the attachment of different groups of TPA and TMDS, like C–N symmetrical elongation, Si–C, and Si–H elongations. The details on all spectra can be found in the SI, section S5.
000 rpm for 10 min. The acetone supernatant was then pipetted into 20 mL scintillation vials. The acetone solvent was evaporated to isolate the reaction product. The isolated yields were obtained, and the purity was determined using 1H NMR (Fig. S15–S22, section S6). All catalytic reaction experiments were performed in triplicate, and the mean of the three measurements was calculated for each condition. The error bars in the figures represent the standard deviation.
Before beginning the catalytic experiments, the catalysts were prepared and activated by removing any moisture present by heating at 100 °C overnight. Liquid propylene oxide (PO) was vaporized inside a pressurized stainless-steel vessel with the liquid supply and vapor outlet placed on its top surface. The vessel was then placed in a water bath that was thermostatted at different temperatures to control the evaporation rate of the PO. To avoid condensation of PO vapors during their transit before entering the reactor, the line was wrapped with a silicone rubber heating tape to maintain a constant and sufficiently high temperature (60 °C). The gaseous stream, consisting of mixtures of high-purity CO2 and vaporized PO with a mole ratio in the range of 1 to 5 and total volumetric flow rates sweeping the range of 13.4 to 14.6 mL h−1, was fed into the packed bed microreactor placed inside a furnace at a temperature between 25 °C and 120 °C, depending on the experiment.
At the end of the test period, the amount of epoxide added to the container was measured and considered as the input PO. Some of the materials in liquid form were deposited in the product while the remaining amount left the system in the form of unreacted gaseous epoxide. The quantity of gaseous epoxide that left the system was determined using mass balance calculations that involved the input PO composition, the amount used to produce the product (based on stoichiometry), and the amount of epoxide measured by 1H NMR, leading to the amount of conversion during the experiment. After the reaction, the content of the reactor was cooled to ambient temperature. Deuterated chloroform was added as a solvent for 1H NMR spectroscopy analysis, the mixture was stirred for another 15 min, and centrifugation was performed to separate the catalyst from the solution. Finally, the reaction products were identified and quantified using 1H NMR spectroscopy. The conversion of propylene oxide was estimated by analyzing the 1H NMR data in combination with mass-balance calculations. This method involves first calculating the integral of the NMR peak for the cyclic carbonate and PO, ensuring that these integrals are normalized based on the number of contributing nuclei, if necessary. The conversion of the cyclic carbonate was then determined using eqn (1). This formula quantitatively reflects the proportion of the cyclic carbonate in the mixture relative to the total amount of both reactant and product and offers a direct insight into the efficiency of the catalytic reaction under study. The turnover frequency (TOF) was calculated as the moles of product formed per mole of catalyst per unit time, which aligns with the principle of quantifying the catalyst's activity over time (eqn (2)).
![]() | (1) |
![]() | (2) |
Control experiments conducted in the presence of only tetrabutylammonium iodide in bulk solution show that very low yields are obtained and that several hydrolysis side products are produced when no Lewis acid catalyst is used.38 Although silica materials do not possess inherent Lewis acids in their structure, the presence of silanol groups on the surface can help stabilize the system by hydrogen bonding to the oxygen atoms of the epoxide and/or activated carbon dioxide.39,40 Although catalysts typically accelerate chemical reactions by reducing the energy of activation of the substrates, it is also possible to accelerate the same reaction by increasing the concentration of the reagents. By exploiting oversolubility, which can increase the local concentration of CO2 by a factor of 7 within the pore structure of mesoporous silica, it is possible to increase a reaction rate without requiring higher pressures.41 To confirm the generality of this process in commercial materials rather than in well-ordered silica, we compared the catalytic activity of SBA-15 and MCM-41 to that of R114, R150, and R170 silica in the conversion of epoxides to cyclic carbonates in the presence of CO2. These latter materials, produced by Silicycle, are irregular silica gels with pores that have diameters in the range of 6 to 7 nm and surface areas in the range of 400–600 m2 g−1. The grafting of 3-iodopropyltrimethoxysilane on these commercial silicas occurred readily and in high yield, offering a coverage of approximately 15% in mass, which is like what was observed with SBA-15 and MCM-41.42 A comparison of the physical properties of silica materials is presented in Tables S1–S5 in the SI. As shown by these data and the spectroscopic characterization that was carried out on all silica materials (see SI), there is no significant difference between the regular (SBA-15 and MCM-41) and irregular (R114, R150, and R170) silicas before and after grafting.
:
1) were necessary when the yields were lower. Control reactions with the ammonium salt were performed to ensure that the catalytic support was necessary to obtain good yields. The results demonstrate that the ammonium salt under similar conditions gives a low yield of 4 ± 4% of the cyclic carbonate under optimal conditions. These findings corroborate studies with the mesoporous silicas MCM-41 and SBA-15, in which acceleration was possible due to the presence of the silica material.34
The yields obtained with catalyst loadings higher than 10% are low for two reasons. First, it was difficult to isolate the styrene carbonate that tends to remain within the pores. Second, the supernatant transfer steps during centrifugation resulted in significant losses. In comparison, the test with a catalyst loading of 0.2 mol% used 2500 mg of the epoxide, which made the purification and yield more satisfactory. However, because this carbonate is soluble in the epoxide, excess styrene oxide can act as a solubilizing agent while also acting as a reagent. Thus, the catalytic system developed using these materials is optimal when using a large quantity of the reagents. As a result, we decided to reproduce the CO2 cyclization reactions using styrene oxide with commercial materials at a catalyst molar ratio of 1%, a temperature of 50 °C, a pressure of 1 bar, and a reaction time of 24 h.
In the next step, we studied catalytic conversion using pristine and passivated materials, as presented in Fig. 4a and b, respectively. These tests were carried out under the optimized conditions of 50 °C and 24 h, but with a silica mass corresponding to that used in the 1 mol% tests. These tests were necessary because the surface of silica materials contains silanol groups, which, through H bridges, can promote the opening of the epoxide and aid in the conversion. However, low conversions were expected because no nucleophiles were present in the reaction medium to catalyze the transformation. This assumption was proven correct based on the results in Fig. 4a. Although materials R114 and R150 yielded only 9 ± 4% and 7 ± 2%, respectively, material R170 yielded conversions of 30 ± 15% even without the anion. Although small-sized silica particles have difficulty achieving conversion, the significant conversion observed with material R170 could be explained by a greater abundance of silanol groups on its surface. Passivated materials were also tested in the catalytic transformation (Fig. 4c). Similar results were obtained for the raw materials, although a slight increase in yields was observed with increasing particle size. Likely, the smaller pore diameters of the R150-TMDS and R170-TMDS materials, 3.9 and 4.2 nm, respectively, instead of 5.8 nm for R140-TMDS, could accentuate the oversolubility effect.34 Thus, the surrounding CO2 crowding is higher, and this has the effect of increasing the rate of the homogeneous uncatalyzed transformation. This hypothesis may explain the average yield of R114-TMDS of 9 ± 2% compared to the yields of 29 ± 12% and 31 ± 8% obtained for R150-TMDS and R170-TMDS, respectively. The TMDS group allows the removal of certain silanol groups by substitution with a silane group SiH(CH3)2, on the surface, but complete passivation of the material is never truly possible, which suggests that certain silanol groups, or even the hydrogen on the TMDS group, may contribute to the observed conversion. It should be noted that the epoxide possesses a high ring strain energy caused by the 60° angles between these atoms, which gives it high reactivity. This “potential” chemical energy, combined with the addition of heat, pressure, and a few hydrogen bonds, can promote epoxide opening even in the absence of an added nucleophile. Fig. 4d presents the catalytic activation of epoxides using TPA-grafted materials under optimal conditions (1 mol%, 50 °C, 24 h). The results of the catalytic cyclization of CO2 to styrene oxide confirm that the ammonium salt is essential to achieve yields greater than 70%. The R114-TPA catalyst yielded 75 ± 6%, R150-TPA yielded 67 ± 8%, and R170-TPA yielded 74 ± 5%. The iodide counterion of the salt promotes activation of the epoxide to open the ring. Compared to control reactions with only the catalyst, the catalytic support, which contains silanol groups and pores of an appropriate size for the supersolubility effect, has a favorable effect on ring opening. Although significant differences were sometimes observed among the yields of the triplicates, we nevertheless have a certain reproducibility of the yields. The commercial silicas, surface-grafted with the ammonium catalyst and passivated with TMDS, were also tested. The R114-TPA-TMDS catalyst yielded 82 ± 6%, R150-TPA-TMDS yielded 74 ± 5%, and R170-TPA-TMDS yielded 76 ± 6%. The TMDS-passivated materials exhibited a yield increase of 6%, 7%, and 2% for the R114-TPA-TMDS, R150-TPA-TMDS, and R170-TPA-TMDS materials, respectively, compared to their catalyst-only counterparts. It is possible that the passivating agent slightly increases conversion. This hypothesis stems from the observation that the starting epoxide is soluble in n-hexane, whereas styrene carbonate is not. Thus, styrene oxide will have a certain affinity for a hydrophobic surface, whereas styrene carbonate, which has a lesser affinity for hydrophobic substances, could be more easily dislodged from the active sites. The excess styrene oxide and its solubilizing effect on styrene carbonate should also help dislodge the formed product from the pores and aid in catalysis.
We tested the synthetic materials MCM-41 and SBA-15 and the grafted analogues under the same conditions to confirm that the irregular silicas are as efficient as the regular ones. The results, shown in Fig. 5a, demonstrate yields lower than those obtained with commercial materials. The yields obtained were 66 ± 24% for MCM-41-TPA and 65 ± 7% for MCM-41-TPA-TMDS, and 61 ± 6% for SBA-15-TPA silica and 70 ± 7% for SBA-15-TPA-TMDS silica. The lower yields with the new catalytic conditions could be explained by the high specific surface area of these MCM-41 and SBA-15 silicas, with specific surface areas ranging from 600 to 1000 m2 and from 400 to 800 m2, respectively.43 This physical characteristic can cause strong adsorption of liquids and require a larger quantity of reagents to disperse and wet these materials. Without the addition of a solvent to produce better homogenization and dispersion of the epoxy on the material, lower yields (than those previously obtained) could be obtained. Fig. 5b shows the yields obtained for the larger-scale reactions (1 mol% of catalyst and 5 g of styrene oxide). Catalyst R114-TPA achieved a yield of over 78% during its first cycle and a better yield of 84% during the second cycle. The efficiencies obtained with the R114-TPA-TMDS catalyst were equally good for all three operating cycles. The efficiency was 80% for the first cycle, 78% for the second cycle, and 83% for the third cycle.
With confirmation of the catalytic efficiency of commercial silica materials for the conversion of styrene oxide to styrene carbonate, we decided to study the efficiency and reactivity using other epoxides and 1 mol% of catalysts R114-TPA and R114-TPA-TMDS under the optimal conditions tested above (Fig. 6). The study of the two catalysts was carried out to determine whether the hydrophilic/hydrophobic surface affinities might cause differences depending on the reagents tested. Terminal epoxides 1 to 7 reacted well, and the two catalytic systems developed from commercial silica R114 proved effective in completing the cyclic carbonate formation reaction. The yields obtained with the terminal epoxides were mostly greater than 70%, except for 4-(fluoromethyl)-1,3-dioxolan-2-one (1) and 4-(bromomethyl)-1,3-dioxolan-2-one (2), which yielded around 50% for both hybrid materials (section S6). One reason for these low yields is epoxide volatility, and losses occur under the combined influence of heat and the gas sweeping flow. However, the reaction products are mainly the corresponding carbonates according to their 1H NMR spectra, which agree with those listed in the literature.44,45
Despite the lower yields of compounds 1 and 2, it is interesting to note that electron-withdrawing groups such as halides do not appear to influence catalytic activity. The yields of compounds 3 to 5, which are known for their electron-donating properties, are also satisfactory, with yields between 68% and 94%. Functional groups such as esters and chlorobenzene in compounds 6 and 7 also do not appear to have an impact on catalytic efficiency.
However, the solid catalyst was markedly less effective for internal or sterically hindered epoxides, since the corresponding carbonates 8, 9, and 10 were not detected by 1H NMR. This behavior likely does not reflect a general intrinsic inactivity of the catalyst, because terminal epoxides bearing a range of electron-withdrawing and electron-donating substituents still afforded moderate to high yields under the same conditions. Instead, the poor reactivity of the internal/hindered substrates is more plausibly attributed to a combination of steric effects and restricted accessibility of the active sites in the porous heterogeneous catalyst. In such cases, bulkier epoxides may undergo less favorable nucleophilic ring opening and may also experience slower diffusion or less effective confinement within the pore network. Accordingly, the present results suggest a substrate-dependent limitation arising from both steric and transport factors, although dedicated mechanistic studies would be required to quantitatively distinguish between these contributions.
As shown in Fig. 7, the 1H NMR data for a cycloaddition reaction performed at room temperature and atmospheric pressure in the packed bed microreactor confirm the observation of two different types of products, namely, the cyclic propylene carbonate (PC) monomer and poly(propylene carbonate) (poly(PC)). Poly(PC) generation is a side reaction that often occurs in heterogeneous systems, even if it was not observed with styrene oxide in our batch experiments. The poly(PC) can be formed either by ring-opening polymerization of propylene carbonate or by the copolymerization of CO2 with PO. This may lead to adsorption or deposition of the polymer onto the catalyst surfaces, thereby blocking active sites. This fouling effect can reduce the catalyst activity over time unless it is mitigated by polymer removal or catalytic reaction design.46 Temperature, time, and catalyst concentration47,48 are factors that can influence the rate of epoxide ring-opening, thus promoting or slowing the growth of the polymer chain towards poly(PC) production.
![]() | ||
| Fig. 7 1H NMR spectra of PC and poly(PC) produced using R170-TPA as catalysts in the micro-reactor at T: 25 °C, P: 1 bar, t: 30 min. | ||
Dilution of the catalyst in an inert matrix was examined as a countermeasure to the loss in selectivity of the catalytic reaction for the targeted monomer.49 The influence of catalyst dilution on the PC/poly(PC) ratio was demonstrated using reduced amounts of the catalyst (R170-TPA) and by adding R170 as a diluent to keep a constant mass in the reactor inventory (Fig. 8). The dilution ratios (massdiluent/masscatalyst) were varied at ratios of 1
:
1, 1
:
2, 1
:
3, and 1
:
4 for both the microreactor (Æ = 0.9 mm) and the centimetric laboratory reactor (Æ = 1 cm) while holding the total inventory mass constant at 75 and 515 mg, respectively. For the conditions described in Fig. 8, the molar flux of CO2 was 40% more than that of PO. Therefore, the reaction was followed in terms of partial PO conversions to PC and to poly(PC). Unwanted conversion of PO to poly(PC) was eliminated in the microreactor if the diluent and catalyst were mixed at a ratio greater than or equal to 1
:
2, whereas higher diluent mass (ratios of 1
:
3 and 1
:
4) resulted in lower conversions to PC (51% and 33%, respectively) versus 80% at the 1
:
2 ratio. The use of catalyst dilution in the centimetric reactor could not completely prevent poly(PC) generation, as reflected in lower PC conversions. However, the two scales having been subject to an identical volume flow rate implies a longer gas residence time in the centimetric reactor (about 2 orders of magnitude) and a consequent loss in selectivity towards the key product (PC). Although RTD was not measured directly in the present work, the comparison between the two reactors can be interpreted considering previous micro-packed-bed hydrodynamic studies from our research group. Prior work has shown that deviations from plug flow in micro-packed beds are generally limited and that near-wall flow can be characterized by locally enhanced velocities arising from the confined geometry.50 These observations are in line with the broader conclusion that micro-packed beds can approach more ideal contacting behaviour than larger packed systems under suitable operating conditions.35 In this context, the much higher conversion observed in the microreactor at very short contact times, compared with the lower conversion observed in the centimetric reactor despite its longer residence time and higher temperature, indicates that reactor performance cannot be explained by residence time alone. Rather, the centimetric reactor likely suffers from broader hydrodynamic non-idealities and stronger external transport limitations, whereas the microreactor operates closer to an apparent kinetic regime.35
Conversely, a significant gain was obtained by favoring the use of microreactors that require lower catalyst quantities and shorter contact times, while the dilution acts as an anti-polymerization barrier. Hence, an effective strategy to suppress this undesired polymerization is to rapidly remove PC product from the reactor before it undergoes further conversion into poly(PC) through parasitic chain-growth processes. However, it should be kept in mind that under the reaction conditions of the test, the reaction products accumulate as a viscous liquid phase that is further trapped by capillary forces within the porous medium. Given the identical micro-mixing quality of the active/inert powders used in both reactors, it is likely that the longer contact times in the centimeter reactor favor mutual diffusion of the PC monomers and thus their polymerization, as demonstrated by analysis of liquid samples after 30 min of reaction.
The best trade-off in terms of selectivity and conversion was achieved with the 1
:
2 powder mixture (Fig. 8). The 1
:
2 dilution ratio is also noteworthy from a practical standpoint, since it reduced the amount of active catalytic material required while preserving high selectivity toward propylene carbonate and suppressing poly(propylene carbonate) formation. This result suggests that catalyst dilution with virgin silica may be a useful strategy not only for hydrodynamic and selectivity control, but also for improving the practical viability of the process.
Although the micro-packed bed exhibited substantially higher conversion and TOF than the centimetric packed bed, this intensification benefit must be interpreted together with the hydraulic penalty intrinsic to micro-structured packed beds. Micro-packed beds are typically associated with large axial pressure gradients because of their small hydraulic diameter and confined pore network, as shown in our previous hydrodynamic studies.35,36,50,51 Their hydrodynamics are also strongly influenced by capillary effects and hysteresis, which further affect pressure-drop behavior under gas–liquid flow.36,51 Therefore, the present comparison should be understood as a performance trade-off: the microreactor offers shorter characteristic diffusion lengths and improved fluid–solid contacting, while the centimetric reactor is less hydraulically demanding but more vulnerable to transport limitations. This interpretation is consistent with prior analyses from our research group showing that confinement and particle-scale hydrodynamics strongly govern reactor behavior in micro-packed bed flow.36,51
Hence, the effect of temperature and reaction time on the cycloaddition reaction catalyzed by the dilute catalyst (1
:
2 ratio) was examined for both reactor scales in the temperature and time ranges of 25 to 120 °C and 30 to 240 min, respectively (Fig. 9). Not surprisingly, the PO partial conversion to PC in the microreactor increased from 80% to approximately 95% when the temperature was increased from 25 °C to 120 °C. However, a temperature above 120 °C led to the formation of side products, which resulted in a significant decrease in product selectivity.52–55 When the reaction was run for 30 min in the centimetric reactor, the conversion to PC was increased from 43% to 68% by increasing the temperature from 25 °C to 120 °C. Although polycarbonate formation was gradually decreased at higher temperatures (up to 120 °C, at which no polymer was observed), some polymerization activity could not be suppressed for a longer reaction time (>30 min).47,56 The significance of selecting an appropriate microreactor becomes unquestionable, particularly when operating at elevated temperatures and short reaction times, thus avoiding the formation and growth of polymeric chains and consequently favoring the selective and entropy-driven production of cyclic carbonate.48
The next operating variable studied was the effect of partial pressure of CO2 on the conversion of PO to PC in both reactors (Fig. 10a and b). The conversion to PC in the microreactor first increased from 80% to 93% when the CO2 pressure was increased by a factor of 4. Beyond this factor, the conversion was reduced, but there was no information on whether the inhibition was due to chemical or physical factors. However, due to the drawbacks of the centimetric reactor enumerated above, although it qualitatively exhibits the same CO2 pressure dependence as the microreactor, it nevertheless achieves much lower PC conversions.
The effect of the molar ratio of CO2 to PO on the PC conversion at constant pressure was evaluated next (Fig. 10c and d). The experiments were conducted over a range of PO evaporation rates (0.4–1.6 mL h−1), whereas the CO2 flow rate was fixed at 13 mL h−1. In the microreactor, an increase in the molar ratio of CO2 to PO from 1
:
1 to 5
:
1 induces a negligible change in the conversion of PC, a quite expected result considering that the equimolecular reaction involves PO as the minority reactant. The centimetric reactor shows atypical behavior in which a stoichiometric excess of CO2 leads to a decrease in PC conversion. This inhibition by CO2 was also found when the partial pressure of CO2 was increased (see Fig. 9a and b and the discussion above).
The residence time (also referred to as contact time) should not be confused with the preset reaction time discussed in connection with Fig. 10a and b; the former is controlled by the total incident flux of reagents. To evaluate the effect of residence time on PC conversion, the volumetric flow rates of evaporated PO and CO2 were adjusted in the ranges of 0.2–4.8 mL h−1 and 2.1–40 mL min−1, respectively, for the microreactor and 1.6–11.2 mL h−1 and 13–90 mL min−1, for the centimetric reactor, while holding constant the molar ratio of the reactants (Fig. 11). The PC conversion in both systems increases with increasing residence time, whereas the turnover frequency (TOF) values decrease (Fig. 11). In addition, the TOF values are much larger in the microreactor (51–715 h−1) than in the centimetric reactor (2–9.1 h−1). If the reaction is kinetically controlled, the residence time and conversion should have a direct relationship.57,58 Thus, if the chemical regime were to prevail in the two reactors while it is subjected to an identical feed composition, then the one with the longer contact time and higher temperature should lead to higher conversions. However, the opposite is observed (Fig. 11). The microreactor converts 85% of the reactants in 2.6 s at 25 °C, compared to less than half (i.e., 40% conversion) during a three-fold greater run time (7.7 s) in the centimeter reactor at 125 °C. Therefore, it is not possible to rule out the negative interference of the external diffusional transport limitations of the reactants and products (as well as hydrodynamic imperfections related to feed distribution and velocity profile developments) on the decrease of conversion in the centimetric reactor, which evidences a rapid cycloaddition reaction for a given catalyst granulometry. If the catalytic reaction is intrinsically rapid, then operation of a miniaturized reactor comes closer to the desirable chemical regime due to the attenuation or complete riddance of external diffusion limitations, in contrast with a cm-scale packed bed reactor. Therefore, it can be concluded that the cycloaddition reaction is controlled by external mass transfer in the case of the centimetric reactor, but that (presumably) an apparent kinetic (at most dependent on intraparticle diffusion limitations) may be in effect in the microreactor.
![]() | ||
| Fig. 11 Effect of residence time on PC conversion in (a) 0.9 mm and (b) 1 cm reactor. CO2/PO (mol mol−1): 1; P: 1 bar, T: 25 °C and 125 °C for the micro- and macro-systems. | ||
To contextualize our findings, Table 1 compares the operational performance of our centimeter- and micrometer-scale systems against established continuous flow reactors reported in the literature. This comparison demonstrates how reactor geometry and scale influence key metrics such as conversion efficiency, selectivity, and overall productivity across different operational regimes.
| Catalyst (type) | Support | Epoxide | Reactor ID | T (°C) | P (bar) | PC yield (%) | Ref. |
|---|---|---|---|---|---|---|---|
| TPA (tethered ammonium iodide) | Commercial silica (R170) | Propylene oxide | 0.9 mm | 25 | 1 | 82 | This work |
| TPA (tethered ammonium iodide) | Commercial silica (R114) | Propylene oxide | 1 cm | 125 | 1 | 70 | This work |
| [bmim]Br | — | Propylene oxide | 2 mm | 140 | 20 | 77.8 | Wu, 2021 (ref. 59) |
| tBu | Amorphous silica | Propylene oxide | 1 cm | 170 | 1 | 50 | North, 2009 (ref. 60) |
| Mesoporous melamine-formaldehyde resin (MMFR) | — | 1,2-Butylene oxide | 1 cm | 120 | 13 | 100 | Bui, 2020 (ref. 61) |
| DBU-based ionic liquid | SBA-15 | Propylene oxide | — | 90 | 20 | 57.10 | Sun, 2021 (ref. 62) |
| Cs–P–Si mixed oxide | — | Propylene oxide | 1 cm | 200 | 80 | 94 | Yasuda, 2006 (ref. 63) |
| MOF-100 (sc) | — | Propylene oxide | — | 100 | 4 | 57 | James, 2018 (ref. 64) |
To comprehensively quantify process intensification, space–time yields were calculated for all reactor configurations, revealing a ∼228-fold improvement in the microreactor compared with batch operation (Table 2).
| Reactor type | Volume (mL) | Residence/reaction time | Yield (%) | STY (mol L−1 h−1) |
|---|---|---|---|---|
| Batch | 10 | 24 h | 75 | 36 |
| Centimetric | 11.78 | 54.2 s | 70 | 45 |
| Microreactor | 0.0955 | 0.44 s | 82 | 8200 |
The following conclusions can be drawn. The cyclic carbonate reaction can be intensified by diluting the catalytic silica powders (to 1
:
2 virgin silica/grafted silica) at room temperature in the microreactor to achieve 80% conversion. However, in the centimetric reactor, only 68% cyclic carbonate conversion was observed at 125 °C. By increasing the pressure from 1 to 3 bar, the conversion in the microreactor was increased from 80% to 92%, in contrast to the centimetric reactor, which displayed much lower performance; from 1 to 5 bar, the conversion increased from 68% to 83%. The residence time can be significantly reduced from several hours in a conventional batch reactor to nearly a minute in a continuous centimeter reactor and to only less than a second in the microreactor for comparable conversions. The external diffusional limitations in terms of CO2 and epoxide mass transfer can be significantly improved by using packed-bed microreactors that provide a closer approach to the chemical regime of catalysts or even the fast ‘intrinsic’ reaction regime.
In this study, we have purposely not addressed issues related to chemical reaction engineering scale-up methodology, such as numbering up a multiple microreactor array. In addition, while the micropacked-bed benchmarking indicates that reactor-scale transport effects contribute to the observed flow performance, we did not complete a full quantitative decoupling of mass transfer from intrinsic kinetics (e.g., via Thiele modulus/effectiveness factor or a comprehensive dimensionless analysis). These experiments, coupled with an effectiveness-factor framework, will be the focus of follow-up work.
Supplementary information is available. See DOI: https://doi.org/10.1039/d6re00100a.
| This journal is © The Royal Society of Chemistry 2026 |