Thomas J.
Neal
a,
Edward D.
Neal
b,
James
Cumby
a and
Jennifer A.
Garden
*a
aEaStCHEM School of Chemistry, University of Edinburgh, Joseph Black Building, David Brewster Road, Edinburgh, EH9 3FJ, Scotland, UK. E-mail: j.garden@ed.ac.uk
bSchool of Chemistry, University of Bristol, Bristol, BS8 1TS, UK
First published on 3rd April 2024
Poly(ε-caprolactone)-poly(lactic acid) (PCL-PLA) copolymers have wide-ranging applications, where the polymer properties are controlled by the chain structure (i.e. block or random). Yet the synthesis of well-defined higher order multiblock PCL-PLA copolymers remains challenging, as competitive transesterification processes can occur that disrupt the polymer structure. Herein, we demonstrate that controlled transesterification can be harnessed as a “top down” method of tailoring PCL-PLA copolymer structures, instigated by the addition of ε-caprolactone to a living PCL-PLA-Zn copolymer chain. The extent of transesterification can be enhanced by increasing the ε-CL stoichiometry and decreasing the chain length of the diblock PCL-PLA precursors. While transesterification decreases the average length of the PCL and PLA blocks, the polymers retained their “blocky” nature as evidenced by DSC analysis. Novel computer simulations on simplified oligomeric systems show that transesterification occurs in both the PCL and PLA blocks of the original copolymer. This methodology also successfully transesterified an isolated PCL-block-PLA copolymer, suggesting that this zinc-catalysed approach may be a versatile post-polymerisation method for diversifying copolymer structures.
In addition to the choice of monomers, the copolymer properties are dictated by the composition and structure. The monomer distribution can vary from completely random to fully segmented block copolymers;24–31 the latter can give nanoscale phase-separation between the individual blocks, which can lead to favourable thermal and mechanical properties.32,33 Yet while the synthesis of PCL and PLA homopolymers via the ring opening polymerisation (ROP) of ε-caprolactone (ε-CL) or lactide (LA) is straightforward to achieve, the synthesis of PCL-block-PLA multiblock copolymers is challenging because transesterification can disrupt the block copolymer structure.34–36 Transesterification is particularly prevalent when extending a PLA* chain (* denotes a living polymer chain) with ε-CL, and very few catalysts have been successful in generating well-controlled di- or tri-block copolymers from PLA*.37,38 We previously reported that catalyst LZn2Et/BnOH (Fig. 1) delivered excellent activity and control in the synthesis of PCL-block-PLA copolymers (i.e. when ε-CL was polymerised first and LA second), yet gave random copolymer structures when ε-CL was added to a living PLA* chain.39
Fig. 1 Synthesis of PCL-PLA diblock copolymers via ROP using LZn2Et/BnOH,39 and the strategy investigated herein to modify the copolymer structure using controlled transesterification. |
Other methods to prepare multiblock copolymers have included the use of diethylene glycol as a bifunctional alcohol initiator to prepare PLA-PCL-PLA triblock copolymers via formation of a PCL homopolymer with two active chain ends; this approach was limited to the formation of triblock copolymers.40 To achieve higher-order PCL-PLA multiblocks, relatively short hydroxy-end capped block copolymers have been reacted with a diisocyanate, to form urethane linkages between the copolymer chains.41 However, this method is often poorly controlled and leads to broad dispersities.
Could transesterification be a friend instead of a foe? The Platel group recently showed that transesterification can deliver tuneable copolymer structures from mixed LA/CL monomer feeds i.e. via a “bottom up” approach.42 Herein, we report an alternative “top down” method that uses a controlled degree of transesterification to tailor the structure of PCL-block-PLA copolymers to generate higher-order multi-block structures. Transesterification is instigated and controlled by the addition of ε-CL to a PCL-block-PLA* chain in the presence of a bis-zinc catalyst. Through novel modelling simulations underpinned by 13C NMR studies, we investigate the microstructures of the resultant PCL-PLA copolymers and show how this methodology can be utilised to modify isolated copolymers.
The resultant copolymer composition, structure, and the extent of transesterification within the targeted PCL100-block-PLA100, PCL200-block-PLA200 and PCL400-block-PLA400 copolymers was investigated using 1H NMR spectroscopy. For PCL100-block-PLA100, integration of the PCL and PLA resonances determined the PCL:PLA composition to be 116:84 (Fig. S2b†), which was comparable to the targeted value. The 1H NMR spectrum also shows distinct resonances for the PCL units that are directly adjacent to PLA units compared to the other PCL units (Fig. S2b†). The relative integrations of these signals can be used to approximate the number average sequence length of each block (lCL and lLA) and the randomness character of the copolymer (R) (see ESI† for details).43 An R value close to 0 suggests a well-defined block copolymer structure whereas an R value close to 1 suggests a random distribution of monomer units. For PCL100-block-PLA100, lCL and lLA were calculated to be 37 and 50, respectively, with an R value of 0.05. These values are close to the theoretical values for PCL100-block-PLA100 (where R, lCL and lLA are calculated to be 0.02, 100 and 100, respectively) suggesting that minimal structure-disrupting transesterification occurs. Intriguingly, the relative integrations remain constant after 24 h at 70 °C (Fig. S3†), suggesting that no additional transesterification occurs without an external source, and that the structure of the living PCL100-block-PLA100* copolymer is stable under these conditions.
Sample | Diblock copolymer | Transesterification | Post-transesterification copolymer structure | |||
---|---|---|---|---|---|---|
Targeted PCL DPa | Targeted PLA DPb | Eq. of ε-CL added | l LA | l CL | R | |
a Conversion of ε-CL was ≥93% in all cases (see Table S1† for additional details). b Conversion of rac-LA was ≥80% in all cases (see Table S1† for additional details). c Calculated using 1H NMR spectroscopy. d 10 equivalents of ε-CL added initially and then another 10 equivalents were added (refer to Fig. S5†). | ||||||
Control | 200 | 200 | 0 | 100 | 101 | 0.02 |
1 | 200 | 200 | 10 | 33 | 21 | 0.08 |
2 | 200 | 200 | 20 | 13 | 10 | 0.18 |
3 | 200 | 200 | 40 | 8 | 7 | 0.26 |
4 | 200 | 200 | 80 | 7 | 6 | 0.30 |
5 | 200 | 200 | 20 | 11 | 9 | 0.20 |
6 | 100 | 100 | 20 | 5 | 5 | 0.42 |
7 | 400 | 400 | 20 | 33 | 27 | 0.07 |
The effect of the initial block length also influences the blockiness of the copolymer structure upon transesterification. This was investigated by adding 20 eq. of ε-CL to PCL100-block-PLA100* (sample 6) and PCL400-block-PLA400* (sample 7). Specifically, higher number-average sequence lengths were achieved when a longer diblock copolymer was used (Table 1 and Fig. 3a). Overall, these results show that the R and l values, i.e. the level of “blockiness” of the resulting copolymer, can be fine-tuned by varying the number of equivalents of ε-CL added to a living PCL-block-PLA-Zn chain as well as the block length of the diblock copolymer precursor. This raises the question: could Zn-mediated transesterification provide a simple method of modifying the copolymer structure from blocky to tailored random copolymers? To answer this, it is important to understand the discrepancy between the number-average sequence length and the true sequence lengths along a polymer backbone.
We therefore probed the polymer structures by quantitative 13C NMR analysis, as the 13C carbonyl resonances are very sensitive to the sequence of monomer units along the PCL-PLA chain (Fig. 4).49,50 With copolymers 1–4, the most intense signals observed were the CCC and LLL triads, where C and L indicate ring-opened caprolactone and lactic acid units (i.e. half a lactide monomer), respectively. The intensity of these resonances suggest that there are some large blocks of PCL and PLA present even after transesterification, which agrees with the observation of two distinct Tg values in the DSC thermograms. However, transesterification is evident, as baseline resonances due to the LCC, CCL, LCL, CLC, LLC and CLL triads were observed with greater intensities than expected for the triblock copolymer. Importantly, the presence of the CLC signal at 170.8 ppm confirms that transesterification has occurred, as this triad requires the disruption of LL units formed through the ring opening polymerisation of a lactide monomer. The lLA and lCL values were also calculated using the triad intensities from the quantitative 13C NMR spectra.35 For example, sample 3 (Table 1) was calculated to have lLA and lCL values of 12 and 10, respectively, which gave relatively good agreement with the values calculated from the 1H NMR spectra (vide supra). The 13C NMR spectra provided further support for increased transesterification upon increasing the quantity of ε-CL added to PCL200-block-PLA200 (Table 1 and Fig. 4). For sample 1 (10 eq. ε-CL), no signals for the CLC or LCL triads were observed, although small baseline signals for the LCC, CCL, LLC and CLL triads were present. Conversely, all the triad signals are observed for sample 4 (80 eq. ε-CL), with an increase in the CLC signal emphasizing a greater degree of transesterification.
Overall, the observation of the CLC and LCL resonances shows that the structure is not completely “blocky”, and there are some individual caprolactone and lactic acid units along the polymer chain. It is important to note that, while useful, the 1H and 13C NMR spectra give information that is an average of the entire system. This means that transesterification may only occur in a fraction of the copolymers with others remaining unaffected. Therefore, polymer sample 3 was separated into different molar mass fractions using SEC, and the R value of each fraction was subsequently examined by 1H NMR spectroscopy (Fig. S9†). To confirm that the copolymer sample had been successfully fractionated, SEC analysis was performed and showed that each fraction had a different peak molar mass (Mp, Fig. S9†). Importantly, the 1H NMR spectra showed the R values to be relatively constant across the molar mass fractions, suggesting that the transesterified copolymer structure is fairly consistent across the copolymer sample.
In order to probe the trade-off between transesterification and ε-CL propagation, we investigated the impact of adding 20 eq. of ε-CL to PLA* homopolymer with a DP of 200 (Fig. S10†). 13C NMR signals for the CCL, LCL, CLC, LLC, and CLL triads confirmed that the ε-CL units have been inserted into the copolymer chain. However, the CCC triad was absent. This suggests that no significant propagation of ε-CL occurs, although the observation of the CCL signal indicates the potential for sequential insertion of two ε-CL monomers. This indicates that transesterification occurs more rapidly than ε-CL propagation, which is further supported by the observation of the LCL triad. On the basis of these results, we tentatively propose that monomer insertion is likely to proceed via insertion of a single ring-opened ε-CL monomer to the PLA* chain (i.e. PLA-CL*), which subsequently initiates transesterification of an exogenous PLA* chain resulting in a shorter PLA* homopolymer and a longer PLA* copolymer with a single ring-opened ε-CL unit inserted into the chain (Fig. S11†). Due to the living nature of these chains, which are capped by Zn, this procedure is repeated until maximum conversion of monomeric ε-CL is reached. If the point along the polymer chain at which transesterification occurs is randomly selected, then the distribution of ε-CL units along the chain will also be random.
We were curious to understand whether transesterification of PCL-block-PLA* disrupted solely the PLA* block, or also the initial PCL block. Therefore, we compared the 1H and 13C NMR spectra produced from the reaction of PLA20* oligomers with 20 eq. of ε-CL, to that of PCL10-PLA20* oligomers with 10 eq. of ε-CL (Fig. 5 and S12†). Oligomers were used as simpler model systems to facilitate analysis of the polymer structure, with a relatively large ε-CL:polymer ratio used to increase the extent of transesterification.
Fig. 5 Expanded 13C NMR spectra of (a) PLA20* with 20 eq. of ε-CL (sample 8) and (b) PCL10-block-PLA20 with 10 eq. of ε-CL (sample 9), showing the respective peak assignments. |
Firstly, 20 eq. of monomeric ε-CL was added to the PLA20* homopolymer. This increased the Mn value from 6.2 kg mol−1 to 11.8 kg mol−1, confirming incorporation of ring-opened ε-CL into the PLA20* chains (sample 8, Table 2 and Fig. S13a†). Significant transesterification occurred, as evidenced by a substantial signal at 4.13 ppm in the 1H NMR spectrum (Fig. S12a†), and CLC triads in the 13C NMR spectrum (Fig. 5a). The resulting copolymer was determined to have a random structure; both lLA and lCL were calculated to be 1 and 2, respectively (by 1H NMR spectroscopy), and the R value was determined to be 1.33. Notably, this value is greater than 1, which indicates a high concentration of alternating sequences (i.e. CLC and LCL).51 This value is also much greater than the R values of copolymers 1–7, despite using a homopolymer precursor rather than a diblock copolymer, corroborating the influence of block length and ε-CL stoichiometry upon the extent of transesterification. As PLA20* has a low chain length, and the stoichiometry of ε-CL:LA is 1:1, ring-opening and insertion of all ε-CL leads to a highly random copolymer structure. A notable difference between the addition of 20 eq. of ε-CL to PLA20* or PLA200* (vide supra) is that the CCC triad is observed in the former, but not the latter. This suggests that the ε-CL:PLAn ratio influences the relative rates of ε-CL propagation vs. transesterification, with an increased quantity of ε-CL promoting propagation.
Sample | (Co)polymer | Transesterification | Post-transesterification copolymer structure | ||||
---|---|---|---|---|---|---|---|
Targeted PCL DP | Targeted PLA DP | Eq. of ε-CL added | l LA | l L | l CL | R | |
a Calculated using 1H NMR spectroscopy and rounded to the nearest integer. b Average sequence length of lactic acid unit, L, which is half an LA unit, rounded to the nearest integer. c Calculated using 1H NMR spectroscopy. | |||||||
8 | — | 20 | 20 | 1 | 2 | 2 | 1.33 |
9 | 10 | 20 | 10 | 2 | 3 | 2 | 1.05 |
Secondly, 10 eq. of ε-CL was added to a PCL10-block-PLA20 oligomer (sample 9, Table 2) and SEC analysis confirmed uptake of ε-CL into the polymer structure (Mn increased from 6.6 kg mol−1 to 9.0 kg mol−1, Fig. S13b†). 1H and 13C NMR analysis confirmed the formation of a random copolymer (lLA = lCL = 2 and R = 1.05, with observation of all eight triads, Fig. 5b and S12b†). Importantly, the relative intensity of both the CCC and LLL resonances was reduced after transesterification with ε-CL. The percentage of ring-opened ε-CL in CCC sequences reduced to 37% (see Fig. S14† for calculation) from 91% (theoretical value of 90%, i.e. 9 PCL units in CCC sequences and 1 in a CCL sequence) after transesterification, and the percentage of LA present in LLL sequences reduced to 52% (see Figure) from 96% (theoretical value of 95%, i.e. 19 PLA units in LLL sequences and 1 in a CLL sequence). If ε-CL was exclusively inserted into the PLA block of the PCL10-PLA20 precursor then the minimum percentage of ε-CL in CCC sequences would be 45% (refer to Fig. S13 in the ESI† for details). Therefore, a reduction to 37% suggests that the PCL block is also disrupted during the transesterification.
DSC analysis of samples 8 and 9 confirmed the highly random post-transesterification structure suggested by the 13C NMR analysis, as only one Tg was observed at −22 °C and −25 °C respectively (Fig. S15†), with no evidence of PCL crystallinity. Additionally, a PCL20-block-PLA20 diblock copolymer was synthesised and used as a reference, which displayed two distinct Tg values (−57 °C and 25 °C) and PCL crystallinity.
Individual sequence lengths for each monomer in the lowest scoring sequences were extracted for samples 8 and 9. To show the frequency with which these sequence lengths occur in the lowest scoring sequences, 2D histograms of sequence number against sequence length were prepared (Fig. 6). These histograms illustrate that there are a high number of low sequence lengths (1–4) present in the majority of the lowest scoring patterns, and that the frequency of sequence lengths present decreases rapidly for higher sequence lengths (>4). The histogram obtained from sample 9 shows a slightly longer tail, which may arise from the lower number of equivalents of ε-CL added compared to sample 8, giving less transesterification. These histograms further demonstrate the randomness of the oligomeric structures produced via transesterification.
Sample | Initial polymer | Transesterification | |
---|---|---|---|
Targeted PCL DP | Targeted PLA DP | Eq. of δ-VL added | |
10 | — | 20 | 20 |
11 | 20 | — | 20 |
1H NMR analysis of copolymer 10 showed a significant resonance at 4.14 ppm, indicative of δ-VL units adjacent to LA units and providing clear evidence for δ-VL initiating transesterification (Fig. 7a).54 The 1H NMR spectra of sample 11 does not provide useful information on transesterification due to overlapping resonances for PCL and PVL. However, the 13C NMR spectrum clearly distinguishes between the different α-carbon environments (i.e. the carbon adjacent to the carbonyl), and four resonances are observed between 63.5–64.5 ppm relating to the VC, CC, VV, and CV diads (V and C represent ring-opened δ-VL and ε-CL units, respectively).55 The presence of these diads confirms that δ-VL can be used to transesterify a PCL homopolymer. As the ring-strain of the cyclic esters decreases in the order LA > ε-CL > δ-VL,53 this may explain why δ-VL can transesterify both PCL* and PLA* homopolymers, and why ε-CL transesterifies PLA* homopolymers, yet LA does not transesterify PCL* homopolymers.
NMR studies combined with novel reverse Monte Carlo simulations of oligomeric copolymer structures showed that transesterification occurs in both the PCL and PLA blocks of the PCL-block-PLA* oligomer precursors to generate highly random structures with low average sequence lengths. The use of computer simulations is a potentially powerful yet currently underused tool for determining and predicting polymer structures, and provides an interesting avenue for future exploration.
The synthesis of targeted copolymer architectures often relies on an understanding of the monomer reactivity ratios and careful catalyst selection i.e. a “bottom up” approach.41 Here, we show that the post-synthesis addition of ε-CL to a living PCL-block-PLA-Zn chain can disrupt block copolymer structures, providing a complementary “top down” route to generate a diverse range of tailored polymer structures. This approach was successfully used in the post-polymerisation modification of an isolated PCL-block-PLA copolymer. Overall, these results indicate that Zn-mediated transesterification can be used as a method of decreasing the average block length, while maintaining a significantly “blocky” structure.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4py00169a |
This journal is © The Royal Society of Chemistry 2024 |