Hideto Tsuji*,
Kazuya Nakayama and
Yuki Arakawa
Department of Applied Chemistry and Life Science, Graduate School of Engineering, Toyohashi University of Technology, Tempaku-cho, Toyohashi, Aichi 441-8580, Japan. E-mail: ht003@edu.tut.ac.jp
First published on 23rd October 2020
Stereocomplex (SC) formation was reported for the first time for enantiomeric alternating copolymers consisting of repeating units with two types of chiral centers, poly(lactic acid-alt-2-hydroxybutanoic acid)s [P(LA-alt-2HB)s]. L,L-Configured poly(L-lactic acid-alt-L-2-hydroxybutanoic acid) [P(LLA-alt-L-2HB)] and D,D-configured poly(D-lactic acid-alt-D-2-hydroxybutanoic acid) [P(DLA-alt-D-2HB)] were amorphous. Blends of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) were crystallizable and showed typical SC-type wide-angle X-ray diffraction profiles similar to those reported for stereocomplexed blends of poly(L-lactic acid) and poly(D-lactic acid) homopolymers and of poly(L-2-hydroxybutanoic acid) and poly(D-2-hydroxybutanoic acid) homopolymers, and of L,L-configured poly(L-lactic acid-co-L-2-hydroxybutanoic acid) [P(LLA-co-L-2HB)] and D,D-configured poly(D-lactic acid-co-D-2-hydroxybutanoic acid) [P(DLA-co-D-2HB)] random copolymers. The melting temperature values and melting enthalpy values at 100% crystallinity for stereocomplexed solvent-evaporated and precipitated P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) blends were correspondingly 187.5 and 187.9 °C, and 98.1 and 91.8 J g−1. Enantiomeric polymer blending of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) can confer crystallizability by stereocomplexation and the biodegradable materials with a wide variety of physical properties and biodegradability are highly expected to be prepared by synthesis of alternating copolymers of various combinations of two types of chiral α-substituted 2-hydroxyalkanoic acid monomers and their SC crystallization.
Recently, the symmetry between PLLA and PDLA or their alternating packing was found to be retained in the SC crystal lattice,48,49 whereas PDLA and PLLA chains were reported to be contained in the SC crystal lattice with a wide PLLA fractions from 30 to 70%.50,51 The elastic modulus of the PLLA/PDLA SC crystalline region (20 GPa) in the direction parallel to the c-axis was higher than that of PLLA or PDLA homo-crystalline regions (14 GPa),52 which should have been originated from the stronger interaction between PLLA and PDLA chains than that between PLLA chains or PDLA chains, as evidenced by atomic force microscopy.53 Also, utilizing hydrogen-bonding, stereo diblock-like PLAs with high stereocomplexationability were prepared from PLLA and PDLA having 2-ureido-4[1H]-pyrimidinone terminal,54 whereas stereo multiblock PLA was synthesized from DL-lactide at ambient temperature using achiral iron complexes.55 The SC formation of lactic acid (LA) and α-amino acid-based enantiomeric random copoly(esteramides), poly(lactic acid-co-alanine)s was reported.56 Utilizing the stereocomplexed PLA nanofibers, highly transparent self-reinforced PLA composites were prepared.57 PLA stereocomplexed materials having different memory shape effects were prepared by network formation or supramolecular formation and incorporation of elastomeric block.58,59
Similar to SC formation between PLLA and PDLA homopolymers, SC formation took place between the enantiomeric PLA-like homopolymers, poly(α-substituted 2-hydroxyalkanoic acid)s (Fig. 1), such as poly(2-hydroxybutanoic acid) [P(2HB)]18 and poly(2-hydroxy-3-methylbutanoic acid) [P(2H3MB)],18 and poly(mandelic acid).60 Hetero SC formation occurred between PLA and P(2HB), P(2HB) and P(2H3MB) with the different chemical structures and opposite configurations. Ternary SC formation took place in the blends of L- and D-configured P(2HB)s and L- or D-configured PLA,18 L- and D-configured P(2H3MB)s and L- or D-configured P(2HB),61 and D-configured PLA, L-configured P(2HB), and D-configured P(2H3MB) [or L-configured PLA, D-configured P(2HB), and L-configured P(2H3MB)],62 whereas quaternary SC occurred in the blend of L- and D-configured P(2HB)s and L- and D-configured P(2H3MB)s.18
Also, SC formation took place in enantiomeric random copolymer blends of poly(L-lactic acid-co-L-2-hydroxybutanoic acid) [P(LLA-co-L-2HB)] (56/44) and poly(D-lactic acid-co-D-2-hydroxybutanoic acid) [P(DLA-co-D-2HB)] (52/48)63 and of poly(L-lactic acid-co-L-2-hydroxy-3-methylbutanoic acid) [P(LLA-co-L-2H3MB)] (47/53) and poly(D-lactic acid-co-D-2-hydroxy-3-methylbutanoic acid) [P(DLA-co-D-2H3MB)] (47/53),64 and the staggered random copolymers, L-configured P(LLA-co-L-2HB) (50/50) and D-configured poly(D-2-hydroxybutanoic acid-co-D-2-hydroxy-3-methylbutanoic acid) (50/50).65 It should be noted that in these cases, all types of monomer units were confirmed to be packed in the SC crystalline lattice by wide-angle X-ray diffractometry (WAXD). This is in marked contrast with normal crystallization of random copolymers, wherein minor monomer units are excluded from and not included in the crystalline regions.
On the other hand, SC formation took place in enantiomeric alternating copolymer blends of poly(L-lactic acid-alt-6-hydroxycaproic acid) and poly(D-lactic acid-alt-6-hydroxycaproic acid)66 and of poly(L-lactic acid-alt-glycolic acid) [P(LLA-alt-GA)] and poly(D-lactic acid-alt-glycolic acid) [P(DLA-alt-GA)].67 These enantiomeric alternating copolymers which formed SC had the repeating or monomer units of lactic acid-6-hydroxycaproic acid or 6-hydroxycaproic acid–lactic acid and of lactic acid–glycolic acid or glycolic acid–lactic acid. In these repeating units, only one type of chiral center from lactic acid units existed. On the other hand, Tabata and Abe synthesized alternating copolymers composed of repeating or monomer units of two types of chiral centers, D,D-configured poly(D-lactic acid-alt-D-3-hydroxybutanoic acid) and L,D-configured poly(L-lactic acid-alt-D-3-hydroxybutanoic acid) and observed the melting temperature (Tm) difference between the two polymers (233 and 83 °C).68
In the present study, we synthesized enantiomeric alternating copolymers of poly(L-lactic acid-alt-L-2-hydroxybutanoic acid) [P(LLA-alt-L-2HB)] and poly(D-lactic acid-alt-D-2-hydroxybutanoic acid) [P(DLA-alt-D-2HB)] (Fig. 1) and report SC formation between alternating copolymer blends of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB). These alternating copolymers are composed of repeating unit of lactic acid-2-hydroxybutanoic acid or 2-hydroxybutanoic acid–lactic acid, which contain two types of chiral centers from lactic acid and 2-hydroxybutanoic acid units (Fig. 1). So, this is the first report for SC formation between enantiomeric alternating copolymers consisting of repeating units with two types of chiral centers. To investigate the physical properties, crystalline species, and crystallization behavior of unblended P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB), and their blends, WAXD, differential scanning calorimetry (DSC), and Fourier transform infrared (FTIR) were carried out.
The singlet peaks seen at 169.0, 69.0, and 16.8 ppm for 13C NMR spectra of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) are attributed to carbonyl, methine, and methyl carbons of LA units, whereas those at 169.9, 73.6, 24.4, and 9.3 ppm are ascribed to carbonyl, methine, methylene, and methyl carbons of 2HB units [Fig. 2(b) and S2†].75,77 In the case of P(LLA-co-L-2HB) random copolymer, triplet peaks are seen for the methylene carbon of 2HB units (24.2 ppm) and the methine carbon of LA units (16.8 ppm), whereas singlet peaks are observed for P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) [Fig. 2(b)]. Also, in the cases of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB), singlet peaks are observed for the carbonyl carbons of 2HB and LA units, whereas in the case of P(LLA-co-L-2HB) random copolymer, dual peaks are seen for carbonyl carbons of 2HB and LA units [Fig. S2(a) and S3(a)†]. The sharp 1H NMR peaks and singlet 13C NMR peaks of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) indicate the fixed circumstances of LA and 2HB units in alternating sequences but not in the various circumstances in random sequences, confirming the successful synthesis of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) alternating copolymers.
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Fig. 2 (a) 1H NMR spectra and (b) 13C NMR spectra of methylene carbon of L-2HB units and methyl carbon of LLA units for P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) alternating copolymers and P(LLA-co-L-2HB) random copolymer in CDCl3. The spectra for P(LLA-co-L-2HB) random copolymer were reproduced from ref. 75 with permission from Elsevier. |
On the other hand, both solvent-evaporated and precipitated P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) blends showed the crystalline peaks at 11.4° (or 11.2°), 19.8° (or 19.5°), 22.9° (or 22.6°). Here, the data outside and inside parentheses are for the solvent-evaporated and precipitated samples, respectively. The diffraction patterns of P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) blends are similar to those of PLLA/PDLA homopolymer SC,78 poly(L-2-hydroxybutanoic acid) [P(L-2HB)]/poly(D-2-hydroxybutanoic acid) [P(D-2HB)] homopolymer SC,79 and P(LLA-co-L-2HB) (56/44)/P(DLA-co-D-2HB) (52/48) random copolymer SC,63 but completely different from that of P(LLA-alt-GA)/P(DLA-alt-GA) alternating copolymer SC with the crystalline peaks at 17.3°, 18.5°, 21.3° (ref. 67) [Fig. 4]. The observed 2θ values of P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) blends are similar to those of P(LLA-co-L-2HB) (56/44)/P(DLA-co-D-2HB) (52/48) random copolymer SC [11.5° (or 11.3°), 20.0° (or 19.6° and 20.1°), 22.9° (or 22.7°), the data outside and inside parentheses are for the solvent-evaporated and melt-crystallized samples, respectively],63 but lower and higher than those for the melt-crystallized PLLA/PDLA homopolymer SC (11.9°, 20.7°, 24.0°)78 and P(L-2HB)/P(D-2HB) homopolymer SC (10.7°, 18.6° and 19.3°, 21.5°),79 respectively. The interplanar distance (d) and crystalline diffraction angle (2θ) values of samples were obtained from Fig. 4, except for P(LLA-alt-GA)/P(DLA-alt-GA) alternating copolymer SC are tabulated in Table S1,† together with those for poly(L-2-hydroxy-3-methylbutanoic acid) [P(L-2H3MB)]/poly(D-2-hydroxy-3-methylbutanoic acid) [P(D-2H3MB)] homopolymer SC.80 The diffraction peak patterns indicate SC formation between P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB), whereas the 2θ and d values exhibit their SC crystalline lattice sizes are very similar to those of P(LLA-co-L-2HB) (56/44)/P(DLA-co-D-2HB) (52/48) random copolymer SC and between those of PLLA/PDLA homopolymer SC and P(L-2HB)/P(D-2HB) homopolymer SC. Very interestingly, comparison between the WAXD profiles of P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) SC and P(LLA-alt-GA)/P(DLA-alt-GA) SC [Fig. 4] reveals that their SC crystal lattice types of enantiomeric LA-based alternating copolymer are completely different.
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Fig. 4 WAXD profiles of solvent-evaporated (SE) and precipitated (Pr) P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) SC, together with solvent-evaporated and melt-crystallized (MC) P(LLA-alt-GA)/P(DLA-alt-GA) alternating copolymer SC,67 solvent-evaporated and melt-crystallized P(LLA-co-L-2HB)/P(DLA-co-D-2HB) random copolymer SC,63 melt-crystalized P(L-2HB)/P(D-2HB) homopolymer SC,79 and melt-crystalized PLLA/PDLA homopolymer SC.78 The main crystalline diffraction angles of SC crystallites for P(L-2HB)/P(D-2HB) homopolymer SC and PLLA/PDLA homopolymer SC are shown with dash-dotted lines and dotted lines, respectively. The data for P(LLA-alt-GA)/P(DLA-alt-GA) alternating copolymer SC, P(LLA-co-L-2HB)/P(DLA-co-D-2HB) random copolymer SC, P(L-2HB)/P(D-2HB) homopolymer SC, and PLLA/PDLA homopolymer SC were adapted from ref. 67, 63, 79, and 78 with permission from American Chemical Society, The Royal Society of Chemistry, American Chemical Society, and Wiley-VCH, respectively. |
The crystallinity (Xc) values of the samples were obtained from the WAXD profiles in Fig. 3(a–c) and summarized in Table S2.† The Xc values of unblended P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) (both nil) are much lower than the purified and melt-crystallized unblended P(LLA-co-L-2HB) random copolymer (56/44) (43.7 and 36.5% for samples, respectively)75 and purified and solvent-evaporated unblended P(LLA-alt-GA) and P(DLA-alt-GA) alternating copolymers [8.1% and nil for P(LLA-alt-GA) and 7.2 and 4.8% for P(DLA-alt-GA)]. On the other hand, the solvent-evaporated and precipitated P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) blends are 66.7 and 60.8%, respectively, which are lower than those reported for the solvent-evaporated and melt-crystallized P(LLA-co-L-2HB) (56/44)/P(DLA-co-D-2HB) (52/48) random copolymer blends (82.5 and 77.7%, respectively),63 but much higher than those reported for solvent-evaporated and melt-crystallized P(LLA-alt-GA)/P(DLA-alt-GA) alternating copolymer blends (20.8 and 29.2%, respectively). The lower Xc values of unblended P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) compared to those of unblended P(LLA-co-L-2HB) random copolymer (56/44) and unblended P(LLA-alt-GA) and P(DLA-alt-GA) alternating copolymers and the lower Xc values of P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) blends compared to those of P(LLA-co-L-2HB) (56/44)/P(DLA-co-D-2HB) (52/48) random copolymer blends can be ascribed to the lower molecular weights of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB). Interestingly, despite the lower Xc values of unblended P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) compared to those of unblended P(LLA-alt-GA) and P(DLA-alt-GA) alternating copolymers, the higher Xc values of P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) blends compared to those of P(LLA-alt-GA)/P(DLA-alt-GA) alternating copolymer blends exhibit that dual chiral centers per a repeating unit in P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) enhanced the crystallizability of the enantiomeric polymers by stereocomplexation compared to one chiral center per a repeating unit in P(LLA-alt-GA) and P(DLA-alt-GA).
Using the ΔHm and Xc of solvent-evaporated (65.4 J g−1 and 66.7%) and precipitated (55.8 J g−1 and 60.8%) P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) blends, ΔHm values at Xc = 100%, i.e., ΔH0m values were estimated to be 98.1 and 91.8 J g−1, respectively. Using the ΔHm and Xc of solvent-evaporated (83.7 J g−1 and 82.5%) and precipitated (74.3 J g−1 and 77.7%) P(LLA-co-L-2HB)/P(DLA-co-D-2HB) random copolymer blends,63 ΔH0m values were evaluated to be 101.5 and 95.6 J g−1, respectively. Also, using the ΔHm and Xc of solvent-evaporated (53.4 J g−1 and 20.8%) and melt-crystallized (67.7 J g−1 and 29.2%) P(LLA-alt-GA)/P(DLA-alt-GA) blends, ΔH0m values were estimated to be 256.7 and 231.8 J g−1,67 respectively, which are much higher than ΔH0m value of poly(glycolic acid) (206 J g−1)82 and PLLA/PDLA homopolymer SC (142 (ref. 83) and 146 (ref. 77) J g−1). Surprisingly, the ΔH0m values of P(LLA-alt-L-2HB)/P(DLA-alt-D-2HB) blends are similar to those of P(LLA-co-L-2HB)/P(DLA-co-D-2HB) random copolymer blends, despite the fact that P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) have higher sequential regularity compared to that of P(LLA-co-L-2HB) and P(DLA-co-D-2HB). This finding can also be explained by the fact that the molecular weights of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) are lower than those of P(LLA-co-L-2HB) and P(DLA-co-D-2HB) random copolymers. The lower molecular weights or increased density of chain terminals of the former should have increased the defects in the crystalline regions, resulting in lower ΔHm and ΔH0m values.
Finally, the present study reveals that even though alternating copolymers with two types of chiral centers per a repeating unit is amorphous, their enantiomeric polymer blending can impose crystallizability by stereocomplexation and it is strongly expected that the biodegradable materials with a wide range of physical properties and biodegradability can be prepared by various combinations of two types of chiral α-substituted 2-hydroxyalkanoic acid monomers. For this purpose, accumulating the information of physical properties and biodegradability of SCs from enantiomeric alternating α-substituted hydroxyalkanoic acid-based polymers with various combinations of chiral monomers is required.
2HB | 2-Hydroxybutanoic acid |
ΔHm | Melting enthalpy |
ΔH0m | ΔHm at Xc = 100% |
DIU | N,N′-Diisopropylurea |
DSC | Differential scanning calorimetry |
Mn | Number average molecular weight |
MC | Melt-crystallized |
Mw | Weight-average molecular weight |
LA | Lactic acid |
P(2H3MB) | Poly(2-hydroxy-3-methylbutanoic acid) |
P(2HB) | Poly(2-hydroxybutanoic acid) |
P(D-2HB) | Poly(D-2-hydroxybutanoic acid) |
P(D-2H3MB) | Poly(D-2-hydroxy-3-methylbutanoic acid) |
PDLA | Poly(D-lactide) or poly(D-lactic acid) |
P(DLA-alt-D-2HB) | Poly(D-lactic acid-alt-D-2-hydroxybutanoic acid) |
P(DLA-alt-GA) | Poly(D-lactic acid-alt-glycolic acid) |
P(DLA-co-D-2H3MB) | Poly(D-lactic acid-co-D-2-hydroxy-3-methylbutanoic acid) |
P(DLA-co-D-2HB) | Poly(D-lactic acid-co-D-2-hydroxybutanoic acid) |
P(L-2HB) | Poly(L-2-hydroxybutanoic acid) |
P(L-2H3MB) | Poly(L-2-hydroxy-3-methylbutanoic acid) |
PLA | Poly(lactide) or poly(lactic acid) |
P(LA-alt-2HB) | Poly(lactic acid-alt-2-hydroxybutanoic acid) |
PLLA | Poly(L-lactide) or poly(L-lactic acid) |
P(LLA-alt-GA) | Poly(L-lactic acid-alt-glycolic acid) |
P(LLA-alt-L-2HB) | Poly(L-lactic acid-alt-L-2-hydroxybutanoic acid) |
P(LLA-co-L-2H3MB) | Poly(L-lactic acid-co-L-2-hydroxy-3-methylbutanoic acid) |
P(LLA-co-L-2HB) | Poly(L-lactic acid-co-L-2-hydroxybutanoic acid) |
Pr | Precipitated |
SC | Stereocomplex |
SE | Solvent-evaporated |
[α] | Specific optical rotation |
Tg | Glass transition temperature |
Tm | Melting temperature |
Xc | Crystallinity |
WAXD | Wide-angle X-ray diffractometry |
Footnote |
† Electronic supplementary information (ESI) available: S1. Experimental section, S1.1. Materials and synthesis, S1.2. Sample preparation, S1.3. Physical measurements and observation, S2. 1H NMR spectra of P(LLA-alt-L-2HB), P(DLA-alt-D-2HB), P(L-2HB), P(LLA-co-L-2HB), and PLLA (Fig. S1), S3. 13C NMR spectra of P(LLA-alt-L-2HB) and P(DLA-alt-D-2HB) (Fig. S2), S4. 13C NMR spectra of P(L-2HB), P(LLA-co-L-2HB), and PLLA (Fig. S3), S5. WAXD profile of N,N′-diisopropylurea (DIU) (Fig. S4), S6. Interplanar distance and crystalline diffraction angle values of samples (Table S1), S7. Crystallinity and thermal properties of samples (Table S2), S8. FTIR spectroscopy (Fig. S5 and Table S3). See DOI: 10.1039/d0ra08351h |
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