Motosuke
Imada
abc,
Yasumasa
Takenaka
*a,
Takeharu
Tsuge
b and
Hideki
Abe
ab
aBioplastic Research Team, RIKEN Center for Sustainable Resource Science, 2-1 Hirosawa, Wako, Saitama 351-0198, Japan. E-mail: yasumasa.takenaka@riken.jp
bDepartment of Materials Science and Engineering, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8502, Japan
cResearch Center, Innovation and Business Development Division, Nippon Shokubai Co., Ltd, 5-8 Nishi Otabi-cho, Suita, Osaka 564-0034, Japan
First published on 14th September 2020
Kinetic modeling is effective in the development of efficient and manageable polymerization systems. Herein, a kinetic model of the group-transfer polymerization (GTP) of an alkyl crotonate using a silicon Lewis acid catalyst having a trialkylsilyl (trimethylsilyl, triethylsilyl, tert-butyldimethylsilyl, or triisopropylsilyl) moiety and various silyl ketene acetals with a corresponding trialkylsilyl moiety as an initiator is developed to understand the polymerization mechanism. The kinetic model quantitatively verifies proposed elementary reactions. When using a trimethylsilyl moiety, the activation energy of the cyclization reaction (a well-known termination reaction in GTP; Ec = 37.8 kJ mol−1) exceeds that of the propagation reaction (Ep = 28.6 kJ mol−1). This reveals that termination reactions are accelerated more than propagation reactions at high temperatures. In addition, comparison of various trialkylsilyl moieties confirmed that the greater bulkiness of the alkyl substituent on the silyl group increases the ratio of the activation energies of the cyclization and propagation reactions.
Recently, we reported the group-transfer polymerization (GTP) method for the homopolymerization of various alkyl crotonates using only an organic acid catalyst, such as N-(trimethylsilyl)bis(trifluoromethanesulfonyl)imide (Tf2NSiMe3), which is a silicon Lewis acid (LA), and 1-trimethylsiloxyl-1-methoxy-2-methyl-1-propene (MTS) as the initiator.8,9 In general, organocatalysis without metal compounds is beneficial for industrial applications because of the well-known advantages of metal-free polymeric products and processes.10,11
However, the alkyl crotonate GTP mentioned above is usually performed at low temperatures (preferably −40 °C or below) because high reaction temperatures, even ambient temperatures, accelerate termination reactions such as cyclization and/or isomerization of propagating chain-end groups.12–15 Briefly, despite the living-polymerization characteristics of GTP, the propagation reaction declines, with the unreacted monomer remaining after the reaction ceases. Consequently, a polymeric material with a molecular weight that is sufficiently large to realize high-performance applications cannot be produced. Furthermore, the requirement of such low temperatures severely limits the application of GTP to industrial processes.16,17
The construction of a kinetic model is an effective approach toward the development of efficient and manageable polymerization systems that operate at high temperatures. The kinetic model quantitatively demonstrates the elementary reactions and provides useful knowledge related to the polymerization mechanism and design of optimum polymerization systems.
Herein, we develop a kinetic model of the GTP of alkyl crotonates using silicon LA catalysts having a trialkylsilyl moiety (Tf2NSiR1R2R3) and various silyl ketene acetals (R1R2R3SKAs) as the initiator. The kinetic model includes monomer activation steps, propagation reactions of living species, and termination reactions of living species. Furthermore, various trialkylsilyl moieties are compared and analyzed to investigate steric hindrance effects.
Matrix-assisted laser desorption/ionization time-of-flight mass spectroscopy (MALDI-TOF-MS) was conducted using an ultrafleXtreme MALDI-TOF spectrophotometer (Bruker Daltonics, Billerica, MA) operated in reflection mode at an accelerating voltage of 20 kV. The samples that underwent MALDI-TOF-MS were combinations of the reaction mixture (2 μL), the matrix (1,8-dihydroxy-9(10H)-anthracenone (dithranol), 10 mg mL−1, 8 μL), and the ionizing agent (sodium trifluoroacetate, 10 mg mL−1, 2 μL) in THF. These samples were deposited on an MTP 384 ground steel target plate TF in a glovebox. External calibration was conducted prior to data acquisition. The detected mass list was extracted using FlexAnalysis software (Bruker Daltonics).
1H and 13C NMR measurements were performed with a Varian NMR system. The samples were dissolved in CDCl3, and 500 MHz 1H NMR and 125 MHz 13C NMR spectra were recorded at room temperature. The data were calibrated against tetramethylsilane (TMS, δ 0.00) and analyzed using the Mnova NMR software.
Entry | [EC]0 (M) | [MTS]0 (M) | [Tf2NSiMe3]0 (M) | Time (h) | Conv.b (%) | M nc (g mol−1) | Đ (Mw/Mn) | v appd (mol L−1 h−1) |
---|---|---|---|---|---|---|---|---|
a Performed on an aluminum block under an argon atmosphere. CH2Cl2 was used as the reaction solvent. b Monomer conversion was calculated from the sum of the weights of the hexane-insoluble and hexane-soluble parts. c Number-averaged molecular weight (Mn) and dispersity (Đ) were determined using conventional GPC against PSt standards in CHCl3. d Apparent rate of monomer consumption during an initial period (vapp) was calculated using the first data point for each condition. | ||||||||
1 | 2.0 | 0.0050 | 0.0050 | 8 | 11.0 | 10000 | 1.17 | 0.0275 |
2 | 24 | 27.2 | 28300 | 1.14 | ||||
3 | 72 | 53.5 | 52800 | 1.29 | ||||
4 | 168 | 54.8 | 58300 | 1.32 | ||||
5 | 2.0 | 0.0100 | 0.0050 | 8 | 18.1 | 12000 | 1.16 | 0.0453 |
6 | 24 | 47.5 | 33300 | 1.14 | ||||
7 | 72 | 83.2 | 58200 | 1.27 | ||||
8 | 168 | 83.5 | 59000 | 1.26 | ||||
9 | 2.0 | 0.0200 | 0.0050 | 3 | 17.9 | 4100 | 1.20 | 0.1195 |
10 | 7 | 40.6 | 11100 | 1.17 | ||||
11 | 16 | 89.1 | 27300 | 1.17 | ||||
12 | 24 | 100.0 | 31500 | 1.14 | ||||
13 | 48 | 99.9 | 31400 | 1.14 | ||||
14 | 72 | 100.0 | 30700 | 1.16 | ||||
15 | 1.5 | 0.0050 | 0.0050 | 8 | 17.0 | 11600 | 1.16 | 0.0319 |
16 | 24 | 39.9 | 37400 | 1.11 | ||||
17 | 72 | 65.1 | 65000 | 1.25 | ||||
18 | 168 | 64.6 | 60400 | 1.28 | ||||
19 | 1.0 | 0.0050 | 0.0050 | 4 | 15.9 | 6800 | 1.21 | 0.0398 |
20 | 8 | 26.7 | 15300 | 1.18 | ||||
21 | 24 | 63.2 | 40100 | 1.18 | ||||
22 | 72 | 75.6 | 52300 | 1.26 | ||||
23 | 1.0 | 0.0025 | 0.0025 | 24 | 23.2 | 24800 | 1.16 | 0.0097 |
24 | 72 | 44.3 | 46900 | 1.28 | ||||
25 | 168 | 46.5 | 48800 | 1.34 | ||||
26 | 1.0 | 0.0025 | 0.0100 | 6 | 18.5 | 20400 | 1.17 | 0.0308 |
27 | 12 | 30.9 | 34500 | 1.18 | ||||
28 | 24 | 43.3 | 47400 | 1.31 | ||||
29 | 72 | 46.3 | 52300 | 1.36 | ||||
30 | 168 | 46.3 | 53700 | 1.34 | ||||
31 | 1.0 | 0.0025 | 0.0400 | 3 | 24.6 | 28600 | 1.19 | 0.0820 |
32 | 6 | 38.2 | 47200 | 1.19 | ||||
33 | 24 | 46.6 | 57000 | 1.33 | ||||
34 | 72 | 52.3 | 58300 | 1.41 | ||||
35 | 168 | 47.6 | 57100 | 1.31 |
Fig. 1 Plausible propagation pathway for the GTP of a crotonate using a silicon LA catalyst (reproduced from Takenaka and Abe8). |
In order to investigate the reaction order for each concentration of the initiator, monomer, and silicon LA catalyst, double-logarithmic plots of vappversus [MTS]0, [EC]0, and [Tf2NSiMe3]0 were fit to straight lines (Fig. 2(a)–(c)). For the initiator, the slope of the straight line drawn using three data points ([MTS]0 = 0.0050, 0.010, and 0.020 M; [EC]0 = 2.0 M; [Tf2NSiMe3]0 = 0.0050 M) (entries 1, 5, and 9 in Table 1) was 1.04 (R2 = 0.97). For the monomer, the slope of the straight line drawn using three data points ([MTS]0 = 0.0050 M; [EC]0 = 2.0, 1.5, and 1.0 M; [Tf2NSiMe3]0 = 0.0050 M) (entries 1, 15, and 19 in Table 1) was −0.53 (R2 = 1.00). For the silicon LA catalyst, the slope of the straight line drawn using three data points ([MTS]0 = 0.0025 M; [EC]0 = 1.0 M; [Tf2NSiMe3]0 = 0.0025, 0.010, and 0.040 M) (entries 23, 26, and 31 in Table 1) was 0.77 (R2 = 1.00). The value of the slope corresponds to the reaction order of each component in the initial period.
Fig. 2 Double-logarithmic plots of apparent rates of monomer consumption during an initial period (vapp) as a function of (a) the initiator, (b) monomer, and (c) silicon LA catalyst. |
The slope of the plot of ln[vapp] vs. ln[MTS]0 in Fig. 2(a) (1.04) suggests that the initial polymerization rate is almost of first order with respect to the initiator concentration. As shown in Fig. 1, this result implies that an initiator or a living polymer chain-end group undergoes a first-order reaction with an activated monomer generated by the coordination of a monomer to a silicon LA catalyst.
A notable feature of this polymerization system, observed from the analysis of the double-logarithmic plots of the apparent rates of the monomer consumption during the initial period, is that the polymerization rate order calculated with respect to the monomer concentration (slope, −0.53) is negative. Furthermore, the rate order with respect to the silicon LA catalyst concentration (slope, 0.77) is less than one, although this polymerization rate should be of first order when considering only the active-species formation from the reaction between one monomer and one catalyst molecule. These peculiar results for the rate orders with respect to both the monomer and silicon LA catalyst concentrations suggest that the monomer reduces the polymerization rate while the silicon LA catalyst is somehow involved in this reduction. As shown in Scheme 1, we can express these peculiar rate orders with respect to the monomer and silicon LA catalyst concentrations by considering that one more monomer can coordinate with the activated monomer (active species) formed by the association of one silicon LA catalyst with one monomer, which leads to the formation of the inactive species.
Fig. 3 Computed structures of (a) adduct A (EC/+SiMe3 = 1/1) and (b) adduct B (EC/+SiMe3 = 2/1) at the B3LYP/6-31G* level. |
This result suggests that, in both adduct A and adduct B, the silicon atom of the silicon LA catalyst and the lone pair on the oxygen atoms of the carbonyl groups interact via the transfer of an electron because the bond lengths between them are sufficiently short.22,23 Therefore, this result can be considered as evidence for the presence of adduct B and adduct A. In addition, because the bond lengths between the silicon and oxygen atoms of adduct B are longer than those between the silicon and oxygen atoms of adduct A, the monomer activation degree of adduct B is lower than that of adduct A. The length of the vinyl bonds of EC in adduct B (C(1b)C(2b) and C(4b)C(5b), 1.346 Å) is less than that in adduct A (C(1a)C(2a), 1.351 Å), although it is slightly longer than that in free EC, unbound to the silicon LA catalyst (1.339 Å). In addition, the length of the carbonyl bonds of EC in adduct B (C(3b)O(1b) and C(6b)O(2b), 1.251 Å and 1.254 Å, respectively) is less than that in adduct A (C(3a)O(1a), 1.280 Å), although it is slightly longer than that in free EC (1.217 Å).
Fig. 4(a) shows the MALDI-TOF-MS spectrum of the obtained reaction mixture. We can observe five series of mass ions (series A to E), all of which have mass-ion intervals corresponding to a repeat unit of m/z = 100 (in agreement with the molecular weight of MC). A detailed analysis of the mass spectrum reveals that the series A polymer corresponds to the structural formula (CH3)2[CH3OC(O)]C–(MC)n−1–CH(CH3)–HCC(OCH3)(OSiMe3), and the series B polymer corresponds to the structural formula (CH3)2[CH3OC(O)]C–(MC)n–H. The former consists of linear living polymers possessing the chain-end structure of a silyl ketene acetal, and the latter consists of protonated forms of the linear living polymers (in addition to protonolysis during the polymerization, the protonated chain ends observed by MALDI-TOF-MS can result from post-polymerization protonolysis, which might occur because of the acidic compounds present in the form of the matrix (dithranol)). The series E polymer is observed as a major component, and it corresponds to the polymer structures shown in Fig. 4(b). The series E polymer is formed by the cyclization reaction of the linear living polymer (series A), a well-known termination reaction in GTP systems. In addition, 13C NMR studies suggest that such a cyclic structure could correspond to a keto-carbon, as shown in Fig. S1.† Furthermore, in the MALDI-TOF-MS spectrum, the series C and D polymers are also confirmed as intermediates of a transition from the series A to series E polymers.
These results reveal that the cyclization reaction of the linear living polymer proceeds with the formation of alcohols such as MeOH and Me3SiOH, which are protic acids, as shown in Fig. 4(b). In addition, the alcohols generated in situ react immediately with the linear living polymer, and the living chain-end is deactivated. This is probably the reason why the polymers observed when polymerization stopped include the polymer of a linear form.
The initiation or propagation step proceeds with the activated monomer (M*) reacting with the initiator (I) or linear living polymer (PLn), respectively. For simplicity, the rate constants of the initiation and propagation reactions were considered to be similar because the structures of the initiator and the chain-end of the linear living polymer were almost the same; therefore, we treated each reaction as the propagation of a living species using the rate constant kp.
In the termination reaction in the presence of a silicon LA catalyst (C), the linear living polymer (PLn) was cyclized to a polymer having a terminal cyclic structure (PCn) with the formation of an alcohol (R′OH). The rate constant of the cyclization reaction is kc. Moreover, the generated alcohol (R′OH) reacts with the linear living polymer (PLn), and PLn is transformed to the deactivated form (PDn). The rate constant of the alcoholysis is ka. In this study, k1 and k2 were defined as k1 = k2 = 102kp, assuming that they were sufficiently large with respect to the polymerization reaction.
For each component, the rate law is expressed using a reaction time (t(s)) as follows (eqn (1)–(7)):
(1) |
(2) |
(3) |
(4) |
(5) |
(6) |
(7) |
The parameter α, which is assumed to be zero in this study, is the relative value of the rate constant of the propagation reaction from the cyclic form (PCn) toward the propagation reaction from the linear living species (PLn). The seven ordinary differential equations generated were solved numerically for all the simulations in this study. Subsequently, the monomer conversion (x (%)) at t(s) was calculated as follows by using solved [M], and [M*] and , which are recovered as free monomers after the polymerization is quenched with methanol, and the initial monomer concentration [M]0 (please note that [M*]0 and are zero):
(8) |
For further investigation of the alkyl crotonate GTP mechanism using a silicon LA catalyst, AdamsBDF curve-fitting analysis using Mathcad software was conducted using the monomer conversion data presented in Table 1, which were acquired under the following conditions: the initial monomer concentration was 1.0–2.0 M, the initial initiator concentration was 0.0025–0.020 M, and the initial silicon LA catalyst concentration was 0.0025–0.040 M. In this analysis, the kinetic parameters shown in Scheme 2 were optimized, as the simulated and experimental data are in good agreement.
Fig. 5 shows the agreement between the simulated and experimental data for the GTP of EC using MTS as the initiator and Tf2NSiMe3 as the silicon LA catalyst at −40 °C. The kinetic model constructed in this study agrees well with actual experiments in that despite the living-polymerization character of the GTP system, the propagation reaction declines, with unreacted monomer remaining. Table 2 summarizes the estimated kinetic parameters. Representative results are as follows: the rate constant of the propagation reaction kp was 0.94 L mol−1 s−1, and the rate constant of the cyclization reaction kc was 1.70 L mol−1 s−1.
Fig. 5 Curve-fitting calculations for the GTP of EC using MTS as the initiator and Tf2NSiMe3 as the catalyst in CH2Cl2 at −40 °C. The symbols represent the experimental data, and the lines represent the simulation results. The experimental data correspond to (a) entries 1–4, (b) entries 5–8, (c) entries 9–14, (d) entries 15–18, (e) entries 19–22, (f) entries 23–25, (g) entries 26–30, and (h) entries 31–35 in Table 1. |
Kinetic parameter | Unit | Value | |
---|---|---|---|
Propagation | k p | L mol−1 s−1 | 0.94 |
Cyclization | k c | L mol−1 s−1 | 1.70 |
Alcoholysis | k a | L mol−1 s−1 | 0.01 |
1st equilibrium | K 1 | L mol−1 | 630 |
2nd equilibrium | K 2 | L mol−1 | 1.4 |
Entry | Temperature (°C) | Time (h) | Conv.b (%) | M nc (g mol−1) | Đ (Mw/Mn) |
---|---|---|---|---|---|
a Performed on an aluminum block under an argon atmosphere. CH2Cl2 was used as the reaction solvent. The conditions were as follows: [EC]0 = 2.0 M, [MTS]0 = 0.0050 M, and [Tf2NSiMe3]0 = 0.0050 M. b Monomer conversion was calculated from the sum of the weights of the hexane-insoluble and hexane-soluble parts. c Number-averaged molecular weight (Mn) and dispersity (Đ) were determined using conventional GPC against PSt standards in CHCl3. | |||||
1 | −30 | 8 | 17.8 | 20100 | 1.16 |
2 | 24 | 36.6 | 45300 | 1.18 | |
3 | 48 | 41.3 | 51400 | 1.24 | |
4 | 72 | 41.3 | 51400 | 1.24 | |
5 | −20 | 2.5 | 10.9 | 11900 | 1.17 |
6 | 5 | 18.4 | 21200 | 1.18 | |
7 | 10 | 27.7 | 33200 | 1.23 | |
8 | 24 | 32.6 | 38900 | 1.32 | |
9 | 72 | 32.3 | 39100 | 1.31 | |
10 | −10 | 2.5 | 14.7 | 17500 | 1.21 |
11 | 5 | 22.3 | 27100 | 1.26 | |
12 | 10 | 24.9 | 30700 | 1.32 | |
13 | 24 | 25.7 | 31100 | 1.33 | |
14 | 72 | 25.6 | 31600 | 1.32 |
AdamsBDF curve-fitting analysis with Mathcad software was conducted using the kinetic parameters estimated at −40 °C (Table 2) and the monomer conversion experimental data presented in Table 3. Using the rate constant estimated at −40 °C (k−40) and the activation energy (E), the rate constant at temperature T (kT) is expressed as kT = k−40exp[(E/R){(1/−40 °C) − (1/T)}], as per the Arrhenius equation. Using the equilibrium constant estimated at −40 °C (K−40) and the standard enthalpy change (ΔH), the equilibrium constant at the temperature T (KT) is expressed as KT = exp[(ΔH/R){(1/−40 °C) − (1/T)} + ln(K−40)], as per the van't Hoff equation. In this analysis, the activation energies (Ep, Ec, and Ea) and standard enthalpy changes (ΔH1 and ΔH2) were optimized, as the simulated and experimental data presented in Table 3 are in good agreement. Fig. 6 shows the agreement between the simulated and experimental data for the GTP of EC under various temperature conditions, and Table 4 lists the estimated parameters. Representative results are as follows: the activation energy of the propagation reaction Ep was 28.6 kJ mol−1, and the activation energy of the cyclization reaction Ec was 37.8 kJ mol−1. This result suggests that as the reaction temperature increased, the ratio of the reaction rate constants for the cyclization reaction toward the propagation reaction increased. Thus, the kinetic model constructed in this study can convincingly explain the actual polymerization behavior.
Fig. 6 Curve-fitting calculations for the GTP of EC using MTS as the initiator and Tf2NSiMe3 as the catalyst in CH2Cl2 at various temperatures (a: −30 °C, b: −20 °C, and c: −10 °C). The conditions are as follows: [EC]0 = 2.0 M, [MTS]0 = 0.0050 M, and [Tf2NSiMe3]0 = 0.0050 M. The symbols represent experimental data, and the lines represent simulation results. The experimental data correspond to (a) entries 1–4, (b) entries 5–9, and (c) entries 10–14 in Table 3. |
Kinetic parameter | Unit | Value | |
---|---|---|---|
Propagation | E p | kJ mol−1 | 28.6 |
Cyclization | E c | kJ mol−1 | 37.8 |
Alcoholysis | E a | kJ mol−1 | 29.8 |
1st equilibrium | ΔH1 | kJ mol−1 | −14.2 |
2nd equilibrium | ΔH2 | kJ mol−1 | −12.2 |
In the kinetic analysis, a reference temperature (Tr), the temperature at which the monomer cannot be consumed fully, was first set for each system, because the kinetic model in this study includes both the propagation reaction and termination reaction, which significantly reduces the monomer consumption. The kinetic parameters (kp, kc, ka, K1, and K2) were estimated at the reference temperature (Tf2NSiEt3/Et3SKA, Tr = 10 °C; Tf2NSitBuMe2/tBuMe2SKA, Tr = 30 °C; Tf2NSiiPr3/iPr3SKA, Tr = 40 °C). AdamsBDF curve-fitting analyses using Mathcad software were conducted using the monomer conversion data presented in Table S1.† In the analyses, the parameter α was set to zero, except for the case of Tf2NSiiPr3/iPr3SKA (α = 0.1). The estimated kinetic parameters are listed in Table 5, and the curve-fitting results are shown in Fig. S2–S4.† In all cases, the simulations reproduced the experimental data well. Next, we attempted to estimate the activation energies of the propagation, cyclization, and alcoholysis reactions (Ep, Ec, and Ea), as well as the standard enthalpy changes for equilibrium in the formation of M* and (ΔH1 and ΔH2) for each system. The analyses were conducted using the estimated kinetic parameters (kp, kc, ka, K1, and K2) at Tr and the monomer conversion data under various temperature conditions (entries 1–4 and 17–36 in Table S1† for Tf2NSiEt3/Et3SKA, entries 37–42 and 55–66 in Table S1† as for Tf2NSitBuMe2/tBuMe2SKA, and entries 67–73 and 86–102 in Table S1† as for Tf2NSiiPr3/iPr3SKA), in the manner described in the preceding subsection. The estimated kinetic parameters (Ep, Ec, Ea, ΔH1, and ΔH2) for each system are listed in Table 6, and the curve-fitting results are shown in Fig. S5–S7.†Fig. 7 shows the relative values of Ep and Ec for each system with respect to those for the Tf2NSiMe3/MTS system.
Tf2NSiEt3/Et3SKA (Tr = 10 °C) | Tf2NSitBuMe2/tBuMe2SKA (Tr = 30 °C) | Tf2NSiiPr3/iPr3SKAa (Tr = 40 °C) | |||
---|---|---|---|---|---|
a The parameter α was set to 0.1 in the case of Tf2NSiiPr3/iPr3SKA. | |||||
Propagation | k p | L mol−1 s−1 | 4.49 | 6.20 | 1.80 |
Cyclization | k c | L mol−1 s−1 | 1.08 | 0.53 | 0.16 |
Alcoholysis | k a | L mol−1 s−1 | 0.45 | 0.45 | 0.10 |
1st equilibrium | K 1 | L mol−1 | 130 | 81 | 71 |
2nd equilibrium | K 2 | L mol−1 | 0.11 | 0.07 | 0.07 |
Tf2NSiEt3/Et3SKA | Tf2NSitBuMe2/tBuMe2SKA | Tf2NSiiPr3/iPr3SKAa | |||
---|---|---|---|---|---|
a The parameter α was set to 0.1 in the case of Tf2NSiiPr3/iPr3SKA. | |||||
Propagation | E p | kJ mol−1 | 31.7 | 37.4 | 40.0 |
Cyclization | E c | kJ mol−1 | 45.7 | 69.7 | 168.7 |
Alcoholysis | E a | kJ mol−1 | 29.2 | 30.5 | 34.8 |
1st equilibrium | ΔH1 | kJ mol−1 | −13.6 | −14.0 | −14.7 |
2nd equilibrium | ΔH2 | kJ mol−1 | −12.2 | −11.6 | −9.6 |
In all cases, Ec was large with respect to Ep, indicating that the acceleration of the cyclization reaction rate with increasing polymerization temperature is greater than that of the propagation reaction. Furthermore, the values of both Ep and Ec increase in the order Tf2NSiiPr3/iPr3SKA > Tf2NSitBuMe2/tBuMe2SKA > Tf2NSiEt3/Et3SKA > Tf2NSiMe3/MTS. The trialkylsilyl group steric hindrance has previously been reported to increase in the order iPr3Si > tBuMe2Si > Et3Si > Me3Si.24,25 Thus, the results of the present study confirm that the steric hindrance of the trialkylsilyl moiety of a silicon LA catalyst and an SKA can affect both the propagation and cyclization reactions of the GTP of alkyl crotonates. Notably, as shown in Fig. 7, the influence of the steric hindrance of the trialkylsilyl moiety is more pronounced for the cyclization reaction than for the propagation reaction. This result suggests that changing the trialkylsilyl moiety is an effective strategy to prioritize the propagation reaction over the termination reaction, which mainly consists of a cyclization reaction, in a certain temperature range. When the initial concentration of each component was fixed to [EC]0 = 2.0 M, [R1R2R3SKA]0 = 0.0050 M, and [Tf2NSiR1R2R3]0 = 0.0050 M, the monomer was fully consumed in the case of Tf2NSiEt3/Et3SKA at −10 °C (entry 32 in Table S1†), Tf2NSitBuMe2/tBuMe2SKA at 15 °C (entries 61 and 62 in Table S1†), and Tf2NSiiPr3/iPr3SKA at 40 °C (entry 73 in Table S1†). However, in the case of Tf2NSiMe3/MTS, full conversion of the monomer could not be achieved even at a low temperature of −40 °C (entry 4 in Table 1).
The constructed kinetic model can convincingly reproduce the experimentally observed polymerization behavior. In addition, the examination of a trialkylsilyl moiety effect on the silicon LA catalyst and initiator revealed that the steric hindrance of the trialkylsilyl moiety strongly affected the elementary reactions, particularly the propagation and cyclization reactions, in this GTP system.
Further investigations on not only the steric factor but also the electronic factor of various silyl moieties of the silicon LA catalyst and initiator are necessary to establish an optimized, efficient, and manageable GTP system for alkyl crotonates.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0py00353k |
This journal is © The Royal Society of Chemistry 2020 |