Zheng Li,
Jianding Chen,
Guijin Zou,
Tongyuan Zhang,
Dafu Wei,
Xiang Xu,
Yong Guan* and
Anna Zheng*
Key Laboratory of Special Functional Polymeric Materials and Related Technology of the Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology, Shanghai 200237, P. R. China. E-mail: yguan@ecust.edu.cn; zan@ecust.edu.cn
First published on 22nd May 2019
A controlled synthesis method of alkyl methacrylate block copolymers such as poly(methyl methacrylate)-b-poly(ethyl methacrylate) (PMMA-b-PEMA), poly(methyl methacrylate)-b-poly(butyl methacrylate) (PMMA-b-PBMA) and poly(ethyl methacrylate)-b-poly(butyl methacrylate) (PEMA-b-PBMA) via living anionic polymerization was innovated with potassium tert-butoxide (t-BuOK) as initiator in tetrahydrofuran(THF) solvent. The sequential anionic copolymerization could be smoothly conducted at 0 °C and the conversion of all monomers reached up to almost 100%. The copolymers were characterized by gel permeation chromatography (GPC), proton nuclear magnetic resonance (1H-NMR), fourier transform infrared spectroscopy (FTIR) and dynamic mechanical analysis (DMA). It was found that all block copolymers were in a narrow MWD while Mw and weight ratio of each block were coincided with the theoretical values and feed ratio. DMA measurement indicated that all the block copolymers have two glass transition temperatures which have proved the certain microphase separation and the partial compatibility of the blocks. The similar results were achieved after changing feed order or addition amount. Furthermore, the reactivity ratio was also studied and confirmed that reactivity ratio of MMA was the largest among alkyl methacrylate. Based on these results, the anionic block copolymerization containing polar alkyl methacrylate monomers at a commercial scale starts to become possible.
Indeed, because of no double bonds in the main chain, the copolymers contained alkyl methacrylate monomer blocks would have excellent properties oil, oxidation and aging resistance. On the other hand, glass transition temperatures of homopolymers would change along with different alkyl methacrylate monomers from −60 °C (laurate methacrylate (LMA)) to 110 °C (isobornyl methacrylate (IBOMA)).13 Copolymer blocks would lead to micro-phase separation and show excellent mechanical properties,14 thus, these types of novel block copolymers would have wide application prospect. In order to control side reactions and structures of polar monomers, low temperatures and some inhibiting ligand have been adopted for anionic polymerization in recent years.15,16 Copolymers contained PMMA blocks such as polyethylene-b-polypropylene-b-PMMA (PE-b-PP-b-PMMA) and PE-b-polyhexene-b-PMMA (PE-b-PH-b-PMMA) have been obtained via anionic polymerization while fluorenyl-amide ligated titanium/methylaluminoxane/2,6-di-tert-butyl-4-methylphenol was used as complex initiating system.17 Poly(1-adamantyl acrylate) (PAdA) and PAdA-b-PMMA block copolymers of narrow MWDs (1.10) were synthesized successfully in THF solvent at −78 °C with sec-butyl-lithium (s-BuLi)/1, 1-diphenylethyl (DPE)/lithium chloride (LiCl), diphenylmethyl potassium (DPMK)/diethyl zinc (Et2Zn) or sodium naphthalenide (Na-Naph)/DPE/Et2Zn as initiator respectively.18 Synthesis of poly(methyl methacrylate)-b-poly methyl (3,3,3-trifluoropropyl) siloxane (PMMA-b-PMTFPS) diblock copolymers was conducted via anionic polymerization initiated by alkyl lithium functionalized by acetal.19 A plug flow reactor was chosen as reaction vessel to synthesize PS-b-PMMA with high molecular weight in THF at −78 °C.20 PS-b-PI-b-PMMA tri-block copolymer was also produced in which PS-b-PI di-block copolymer polymerized in toluene at room temperature firstly and then the anionic polymerization of MMA was carried out at −78 °C after LiCl/THF adding to the system.21 Moreover, anionic polymerization of dendrimer-like star-branched poly(tert-butyl methacrylate)s (PtBMA) and their block copolymers were also studied at −78 °C.22 However, the polymerization was conducted at low temperatures or initiated by complex and expensive compound which could not be realized in industrialized conditions, which limited the further application.
Our research group has made great efforts on anionic polymerization of polar monomers to explore chain initiation and inhibit side reactions at ambient temperature. A compound so called “P-Complex”23 was synthesized by our group and used as an effective inhibitor to control the side reactions in the anionic polymerization of MMA and its copolymers. Followed the research above, PI-b-PMMA and PBMA-b-PMMA with about 1.2 of MWD were obtained successfully at 0 °C when using n-butyllithium (n-BuLi) as initiator and “P-Complex” as inhibitor.24 The triblock copolymer PS-b-PI-b-PMMA25 was gained and the anionic polymerization was conducted in hydrocarbon (CH) solvent with trace amounts of THF as a polar regulator. Especially, the reaction temperature of MMA was elevated to 0 °C. The structure of PS-b-PI-b-PMMA was compared with predicted and showed obvious microphase separation according to measurement. A counter ion exchange initiating system potassium tert-butoxide (t-BuOK)/n-BuLi26 was researched for anionic polymerization of alkyl methacrylate. Then block copolymer PMMA-b-PtBMA was achieved in THF solvent at the temperatures ranging from 0 °C to 40 °C. It has been shown that t-BuOK was an effective initiator for anionic polymerization of alkyl methacrylate27,28 but whatever it was controlled for anionic polymerization has not ever deeply researched.
Therefore, a series of copolymers containing PMMA, PEMA and PBMA blocks were prepared via anionic polymerization with t-BuOK as initiator in THF solvent at ambient temperature. The conversions of monomers were also focused. GPC, 1H-NMR and DMA measurement were used to investigate the Mw and the structures of gained copolymers. These results were summarized and compared with the theoretical values to confirm this initiating system would be a controlled method for alkyl methacrylate block copolymers. Furthermore, the reactivity ratio measurement of alkyl methacrylate was also carried out and discussed.
1H-NMR spectra was measured by a BRUKER AV400 spectrometer with CDCl3 as solvent and tetramethyl silane (TMS) as the internal reference.
Fourier transform infrared spectroscopy (FTIR) was measured by Nicolet 6700 spectrometer over the wave number range of 4000–400 cm−1.
Dynamic mechanical spectrometer (Q800, TA Co., USA) was used to study the dynamic mechanical properties of the copolymers. The samples were transited into high elastic state by raising temperature and then poured into rectangular strips with size of 30 mm × 12 mm × 3 mm, tested with single cantilever bending mode and heated from −10 to 125 °C, at heating rate of 10 °C min−1 and frequency of 0.5 Hz in a nitrogen atmosphere.
Determination of monomer reactivity ratios was carried out by using the extended Kelen–Tüdos method.
# | Polymer | Mn (×10−3) | MWD | Yield (%) | Eff.b (%) |
---|---|---|---|---|---|
a VTHF = 50 ml, Ct-BuOK = 0.060 mol L−1, Cmonomer = 0.942 mol L−1.b Initiator efficiency (I*) = Mn(calcd)/Mn(obsed), where Mn(calcd) = MW(monomer) × [monomer]/[initiator] × conversion% + MW of chain end groups. | |||||
1 | PMMA | 3.31 | 1.22 | 99.40 | 45.65 |
2 | PEMA | 4.67 | 1.18 | 98.38 | 43.03 |
3 | PBMA | 5.04 | 1.14 | 98.79 | 42.25 |
The PMMA, PEMA and PBMA were synthesized via anionic polymerization with t-BuOK as initiator. The GPC results confirmed the polymers were kept in a narrow MWD and high yields. Obviously, for the existence of association state in t-BuOK solution, the initiator efficiency was not close to 100% but at a stable number of approximately 43% at this situation, which has been discussed in our previous work.27,28 This consequence would provide a possibility of a controlled method for block copolymers of alkyl methacrylate.
On the other hand, in order to determine the reaction time of each block polymer, the kinetic of alkyl methacrylate monomers was studied with t-BuOK as initiator. The results of reaction time were summarized in Table 2 while three monomers were of the same molar amount. The reaction rate of MMA was obviously slow where the conversion of MMA was nearly 100% until about 150 min (Fig. 1). Considering the reaction temperature was at ambient temperature and yields were almost complete, a grand development has been achieved to the previous study.
# | Monomer | mt-BuOK (g) | Ct-BuOK (mol L−1) | Conversion at 35 s (%) | End time (s) |
---|---|---|---|---|---|
a CMMA = CEMA = CBMA = 0.942 mol L−1. | |||||
a | MMA | 0.345 | 0.061 | 1.10 | 9000 |
b | EMA | 0.340 | 0.060 | 78.60 | 108 |
c | BMA | 0.339 | 0.060 | 83.33 | 96 |
While the reactions were terminated at 35 s by CH3OH, the conversion of each monomer was measured. Contrary to the result of MMA, other two monomers EMA and BMA had quite faster reaction rates (Fig. 2). According to classical theory, MMA has the shortest carbon chain length and largest polarity among three monomers so that MMA should have the fastest reaction. Reaction rate would decrease in the order of carbon chain length; however, our research results were poles apart from the prediction. At the same time, in the previous study,26 the reaction rate of t-BMA was ten times faster than that of MMA when the polymerization was initiated by n-BuLi/t-BuOK initiating system, as a collateral evidence.
As we all known, K+ as the counter ion would had positive electrical property reduce a lot instead of Li+ controlling the distance much bigger between ion pairs. On the other hand, comparison among three monomers' size obviously MMA < EMA < BMA. According to the “Ion Pair Channel Idea”,29 the required space for MMA to insert into was least, nevertheless, the difference between channel space of ion pairs and MMA's required space was much huge, causing the reaction rate of MMA the slowest. The required space increased in the order of EMA and BMA which grown closer to the distance between K+ and anion, so it's reasonable that reaction rate become faster.
According to the results above, the reaction time of each block polymer was determined: 3 h for the PMMA block while 0.1 h for the PEMA and PBMA blocks.
# | Polymer | C1 (mol L−1) | C2 (mol L−1) | Time (h) | Mn (×10−3) | MWD | Yield (%) | Wtn1:Wtn2 | |
---|---|---|---|---|---|---|---|---|---|
Calcd | Obseda | ||||||||
a Calculated by 1H-NMR. | |||||||||
4 | PMMA-b-PEMA | 0.941 | 0.942 | 3 + 0.1 | 7.32 | 1.22 | 98.5 | 46.7:53.3 | 46.2:53.8 |
5 | PEMA-b-PMMA | 0.942 | 0.943 | 0.1 + 3 | 7.41 | 1.26 | 97.6 | 53.3:46.7 | 53.3:46.7 |
6 | PMMA-b-PEMA | 0.941 | 1.885 | 3 + 0.1 | 9.78 | 1.28 | 99.0 | 63.1:36.9 | 64.1:35.9 |
7 | PMMA-b-PBMA | 0.942 | 0.942 | 3 + 0.1 | 8.48 | 1.33 | 97.8 | 42.0:58.0 | 40.8:59.2 |
8 | PBMA-b-PMMA | 0.942 | 0.943 | 0.1 + 3 | 8.12 | 1.28 | 98.4 | 58.7:41.3 | 57.5:42.5 |
9 | PMMA-b-PBMA | 0.943 | 1.884 | 3 + 0.1 | 11.05 | 1.21 | 98.1 | 58.5:41.5 | 57.9:42.1 |
10 | PEMA-b-PBMA | 0.942 | 0.943 | 0.1 + 0.1 | 10.93 | 1.26 | 99.2 | 44.5:55.5 | 45.0:55.0 |
11 | PEMA-b-PBMA | 0.942 | 1.882 | 0.1 + 0.1 | 14.72 | 1.36 | 97.5 | 61.0:39.0 | 61.9:38.1 |
The MWD of block copolymers extended to 1.25–1.30 which was slightly larger than that of homopolymers. Considering there were no ligand and the temperature was at 0 °C, the MWD of block copolymers was rather narrower than other copolymers synthesized by different method.3 Taking the sample 4, 7 & 10 GPC curves as examples (Fig. 3), the Mn of copolymers from GPC results was rather close to the calculated ones (the initiator efficiency of t-BuOK was set as 43.5% at this condition) and the yield still reached up to 100%, which was a great breakthrough for anionic polymerization of MMA and other alkyl methacrylate. The GPC results showed a significant single peak distribution and the peaks moved to the left of shorter elution time along with the larger molecule weight. This phenomenon strongly confirmed the copolymers were strict block copolymers.
1H-NMR spectrum of three block copolymers such as PMMA-b-PEMA (sample 4), PMMA-b-PBMA (sample 7) and PEMA-b-PBMA (sample 10) were revealed as typical examples to analyze the structures of block copolymers in Fig. 4. Some peaks at δ 3.58 (a) assigned to protons of methoxy group (–OCH3) in PMMA blocks. Furthermore, a signal at δ 4.02 (b) attributed to protons of methylene connected with the ester group (–OCH2–) and the signal at δ 1.25 (d) corresponded to the protons of the methyl at the end of side chain (–CH3) in PEMA blocks. Besides, there were a peak at δ 3.96 (c) attributing to protons of methylene connected with the ester group (–OCH2–) and a signal at δ 1.60 (e) belonged to the second methylene at the side chain (–CH2–) in PBMA blocks.
Calculating the ratio of the integral areas of these characteristic peaks, the mole ratio of each block could be figured out as showed in Table 3. For example, in sample 4, the mole ratio of MMA and EMA was 1:1.02, which was approximate to the theoretical value (1:1). Naturally, the weight ratio of PMMA and PEMA was worked out 46.2:53.8, closed to the feed ratio (46.7:53.3). Expectedly, the weight ratios of other samples approached to the feed ratios while feed order or additive amount was changed. These results proved quietly little side reaction existed during the anionic polymerization of alkyl methacrylate and the conversions of each block were completed. The block copolymers of alkyl methacrylate monomers were synthesized successfully in a controlled method with t-BuOK as initiator which the final products accorded with the theoretical calculation.
Compared sample 4 & 6, 7 & 9 and 10 & 11 while all the later samples doubled the addition of the first block, the observed Mn increased with the addition of monomers were closed to the calculated. After exchanging the addition order of monomers with the same concentration, all reactions were nearly completed and the Mn almost unchanged. These any anions of three kinds of alkyl methacrylate monomers (MMA, EMA & BMA) could initiate each other. Whatever the concentration or order of monomers was changed, the copolymers could be always gained with narrow MWDs, high yields and Mn which could be designed.
The structure of block copolymers was confirmed by FTIR and Fig. 5 showed the FTIR spectra of sample 4, 7 & 10. Because three copolymers were almost same in structure except the side chain, there were several common peaks in spectra. The absorption bands at 2956.8 cm−1 belonged to methyl (–CH3) vibration in main chains. The bands at 1723.1 cm−1 and 1143.2 cm−1 resulted from the carbonyl (CO) and –C–O– stretching vibration of ester group in blocks. On the other hand, there was no peak at 3185 cm−1 which attributed to tert-butyl (–C(CH3)3) of t-BuOK.30 This phenomenon mean that few initiator remained in the copolymers after treatment.
To analyze the dynamic mechanical behavior of block copolymers, the glass transitions of sample 4, 7 & 10 were measured by DMA. For indicating the glass transitions temperatures clearly, the three curves of loss tangent were plotted in the same figure (Fig. 6). Obviously, in any copolymers, there are two glass transitions which confirmed the copolymers synthesized were definite block copolymers. In the PMMA-b-PEMA copolymer, there are two peaks in tanδ curves, where peak A belongs to PEMA blocks at 70.1 °C and peak B at 83.1 °C indicated the Tg of PMMA blocks. Similarity, peak C (41.2 °C) was attributable to Tg of PBMA blocks and peak D (82.4 °C) was assigned to PMMA blocks in PMMA-b-PBMA. Especially, there are two close peaks in the DMA curves of PEMA-b-PBMA where peak E belongs to PBMA blocks at 49.2 °C and the temperature at peak F (59.2 °C) was Tg of PEMA blocks.
Indeed, on the basis of our GPC and 1H-NMR results above,the Mw of PMMA, PEMA and PBMA blocks in three copolymers would be nearby, however, the glass transition temperatures of same blocks in different copolymers have a certain difference. For a more intuitive presentation of comparison, the data was listed in Table 4. Taking PMMA blocks as example, according to literature and book,31 after calculated using eqn (1):
(1) |
PMMA | PEMA | PBMA | ||
---|---|---|---|---|
Tg (obs) (°C) | PMMA-b-PEMA | 83.1 | 70.1 | — |
PMMA-b-PBMA | 82.4 | — | 41.2 | |
PEMA-b-PBMA | — | 59.2 | 49.2 | |
Tg (cal) (°C) | ∼95 | ∼65 | ∼21 |
All the results above confirmed that a series of well-defined diblock copolymers were synthesized successfully. Considering the temperature was at 0 °C and t-BuOK was used as single initiator without any ligand, this method would have potential of industrialization.
In addition, for the present living anionic copolymerization, only data at relatively high conversion could be obtained due to the very high reaction rate. The extended Kelen–Tüdós method was thus used to determine the monomer reactivity ratios.
Controlling the conversions between 15% and 30% and different molar ratio, a series of copolymers with different units were gained for reactivity ratio measurement. Moreover, the extended Kelen–Tüdós method is expressed by the following equations:
(2) |
(3) |
(4) |
On the other hand, it was observed that –OCH2– and –OCH3 resonances do not split while varying the composition of copolymer PMMA-c-PEMA, leading to sharp peaks at 4.02 (b) and 3.58 (a), respectively. Therefore, the composition of copolymer samples was determined by direct integration of these two signals and the results of Kelen–Tüdós parameters were summarized in Table 5. While the α was calculated as 1.323, the linear regression equation is ‘η = 2.05ε − 1.29’ (Fig. 7) and the intercepts at ε = 0 and ε = 1 of the ε versus η plot gives rEMA = 0.76 and rMMA = 1.71, respectively.
No. | m1 & m2 | Vm1 (ml) | Vm2 (ml) | R | ρ | G | H | η | ε | α |
---|---|---|---|---|---|---|---|---|---|---|
1 | EMA & MMA | 7 | 3 | 1.978 | 1.342 | 0.502 | 2.919 | 0.118 | 0.689 | 1.323 |
2 | 6 | 4 | 1.271 | 0.865 | −0.207 | 1.880 | −0.065 | 0.587 | ||
3 | 5 | 5 | 0.848 | 0.521 | −0.782 | 1.382 | −0.290 | 0.511 | ||
4 | 4 | 6 | 0.565 | 0.374 | −0.962 | 0.863 | −0.441 | 0.395 | ||
5 | 3 | 7 | 0.363 | 0.227 | −1.288 | 0.600 | −0.671 | 0.312 | ||
6 | BMA & MMA | 7 | 3 | 1.569 | 0.500 | −1.569 | 4.922 | −0.222 | 0.697 | 2.141 |
7 | 6 | 4 | 1.008 | 0.332 | −2.047 | 3.082 | −0.392 | 0.590 | ||
8 | 5 | 5 | 0.672 | 0.225 | −2.384 | 2.055 | −0.568 | 0.490 | ||
9 | 4 | 6 | 0.448 | 0.143 | −2.753 | 1.435 | −0.770 | 0.401 | ||
10 | 3 | 7 | 0.288 | 0.089 | −2.949 | 0.933 | −0.959 | 0.303 | ||
11 | EMA & BMA | 7 | 3 | 2.941 | 2.572 | 1.797 | 3.366 | 0.381 | 0.714 | 1.349 |
12 | 6 | 4 | 1.891 | 1.714 | 0.785 | 2.091 | 0.228 | 0.608 | ||
13 | 5 | 5 | 1.260 | 1.171 | 0.183 | 1.358 | 0.068 | 0.501 | ||
14 | 4 | 6 | 0.840 | 0.762 | −0.265 | 0.929 | −0.116 | 0.408 | ||
15 | 3 | 7 | 0.540 | 0.547 | −0.460 | 0.540 | −0.243 | 0.286 |
Similarly, –OCH2– and –OCH3 resonances did not split while varying the composition of copolymer PMMA-c-PBMA. The sharp peaks at 3.96 (c) and 3.58 (a) could still determine the composition of copolymer samples. While the α was calculated as 2.141, the linear regression equation is ‘η = 1.90ε − 1.52’ (Fig. 7) and the intercepts at ε = 0 and ε = 1 of the ε versus η plot gives rBMA = 0.38 and rMMA = 3.26, respectively.
At this moment, it is important to point out that such a difference in the monomer reactivity ratio (0.38:3.26) might indicate that the early polymer must be close to PMMA in character and the later be virtually PBMA, so the opportunity for long chain segment or little block polymer would occur in the intermediate region and to a relatively small extent.33 When 1H-NMR of PMMA-b-PBMA and PMMA-c-PBMA at 30% conversions were compared in Fig. 8, it is obvious that δ 3.96 (c) and δ 3.58 (a) are the signals attributed to the PMMA and PBMA blocks. It is confirmed that little block polymer occurred in the random polymers. Additionally, the multiplet peaks around main peak were caused by different chemical environment among the block chains. This result proved the reactivity ratio corrected in one way.
However, there were overlaps between peaks at δ 4.02 (b) and δ 3.96 (c) and it was hard to vary the composition of copolymer PEMA-c-PBMA. Fortunately, the signals at δ 1.25 (d) and δ 1.60 (e) belonged to –CH2– in side chains could be used to determine the composition of copolymer samples. While the α was calculated as 1.349, the linear regression equation is ‘η = 1.56ε − 0.69’ (Fig. 7) and the intercepts at ε = 0 and ε = 1 of the ε versus η plot gives rEMA = 0.87 and rBMA = 0.93, respectively. It is natural that reactivity ratio was closed for the similar polarity and structures.
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