Hans R.
Kricheldorf
*a and
Steffen. M.
Weidner
b
aUniversity of Hamburg, Institute for Technical and Macromolecular Chemistry, Bundesstrasse 45, D-20146 Hamburg, Germany. E-mail: hrkricheldorf@aol.de
bFederal Institute for Materials Research and Testing–BAM, Richard Willstätter Strasse 11, D-12489 Berlin, Germany
First published on 14th August 2025
The usefulness of various N- and P-based catalysts for syntheses of cyclic polyglycolide via zwitterionic polymerization of glycolide was examined. Most catalysts produced discolored, largely insoluble polyglycolides consisting of cycles and unidentified byproducts. Soluble, cyclic polyglycolides were obtained using neat pyridine as catalyst at 120 °C, 100 °C, 80 °C, and even at 60 °C. The number-average molecular weights were extremely low and depended slightly on the glycolide-to-pyridine ratio. Three different mass distributions of the cycles were detected by mass spectrometry, depending on the reaction conditions. The cyclic polyglycolides were also characterized by differential scanning calorimetry (DSC) and small-angle X-ray scattering (SAXS) measurements. The SAXS data in combination with the mass spectra indicate that the majority of the cycles form extended-ring crystallites.
Version II is characterized by ring-opening polymerization (ROP), which yields reactive linear intermediates that undergo polycondensation and cyclization simultaneously. This version is called the ROPPOC (Ring-Opening Polymerization with Polycondensation and Cyclization) method. As defined and illustrated in a previous review,13 the ROPPOC method may involve ionic or covalent end groups. The variant with two ionic end groups is called zwitterionic polymerization (ZP). The first formulation of a zwitterionic polymerization mechanism was the polycondensation mechanism proposed by Elias and Bühler in 1970 (see Scheme 1), which was not supported by any experimental evidence.14,15 Four years later, Kricheldorf reported the first formulation and realization of a zwitterionic ring-opening polymerization (ROP) based on the pyridine-catalyzed ROP of proline N-carboxyanhydrosulfide (NTA, Scheme 2).16
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Scheme 1 Zwitterionic polycondensation mechanism formulated in ref. 15 for the trialkylamine-catalyzed polymerization of thioglycolic acid S-carboxyanhydride (1,3-oxathiolane-2,5-dione). |
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Scheme 2 Mechanism of a pyridine-catalyzed zwitterionic polymerization of proline N-carboxy anhydrosulfide formulated in ref. 16. |
Further pyridine-catalyzed ROPs of N-carboxyanhydrides (NCAs) and N-thiocarboxyanhydrides (NTAs) of various amino acids were also performed,17 but the cyclic architecture of the resulting polypeptides was not evident at that time. However, a re-investigation of previous experiments, as well as new experiments involving various amino acid NCAs, proved the cyclic topology by means of MALDI-TOF mass spectrometry in 2005 and 2006.18–20 Earlier, the first author had studied pyridine- and trialkylamine-catalyzed polymerizations of S-carboxyanhydrides of mercaptoacetic acid and mercapto-D,L-lactic acid.21,22 Although a zwitterionic mechanism was not formulated, a detailed reinvestigation in 2007 proved that poly(thioglycolide) and poly(thio-D,L-lactide), prepared in this manner, indeed had a cyclic topology due to a zwitterionic polymerization mechanism.23 Further cyclic polyesters were prepared by pyridine-catalyzed ROPs of hydroxy acid O-carboxyanhydrides.24–26 Cyclic anhydrides and anhydrosulfides are strong electrophiles that are sensitive to traces of pyridine and substituted pyridines. However, pyridines are not reactive enough to catalyze zwitterionic polymerizations of cyclic esters, which are far less electrophilic, such as δ-valerolactone, ε-caprolactone, and cyclic carbonates. N-heterocyclic carbenes and amidines are effective zwitterionic catalysts for these monomers, as demonstrated by Waymouth et al.27–33 However, the high basicity of these catalysts causes racemization of L-lactide at room temperature. Thus, these catalysts are ineffective for preparing optically pure cyclic poly(L-lactide). This disadvantage is, of course, not relevant for other cyclic esters. Zwitterionic polymerizations of lactide by modified carbenes and other catalysts have also been reported by other research groups.34–38
Glycolide is the most reactive cyclic ester commercially available. Beginning with the work of Gilding and Reed,39 it was found that its incorporation rate is far higher than that of lactide when the two monomers are co-polymerized. Furthermore, racemization is not a problem. Thus, the authors investigated whether zwitterionic polymerizations of glycolide could be catalyzed by nucleophilic tertiary amines or phosphines at temperatures above 100 °C in bulk (Scheme 3).
The polymerizations catalyzed by DMIM (0.1 mmol) or TPP (0.1 mmol) were conducted analogously.
The GPC measurements were performed in a modular system kept at 30 °C consisting of an isocratic pump (Agilent, USA) running with a flow rate of 0.5 mL min−1 and a refractive index detector (RI-501-Shodex). HFIP was used as eluent. Samples were manually injected (100 μL, ca. 2–4 mg mL−1). For instrument control and data calculation WinGPC software (Polymer Standard Service-PSS now Agilent, Mainz, Germany) was used. The calibration was performed using a polymethylmethacrylate (PMMA) standard set (Polymer Standards Service – PSS, Mainz).
The DSC heating traces were recorded on a (with indium and zinc freshly calibrated) Mettler-Toledo DSC-1 equipped with Stare Software-11 using a heating rate of 10 K min−1. Only the first heating traces were evaluated.
The SAXS measurements were performed using our in-house SAXS/WAXS apparatus equipped with an Incoatec™ X ray source IμS and Quazar Montel optics. The wavelength of the X ray beam was 0.154 nm and the focal spot size at the sample position was 0.6 mm2. The samples were measured in transmission geometry and were recorded with a Rayonix™ SX165 CCD-Detector. The SAXS measurements were performed at sample-detector distance of 1.6 m and the accumulation was 1200 s for each position. DPDAK, a customizable software for reduction and analysis of X-ray scattering data sets was used for gathering 1D scattering curves.40 For the evaluation of the crystallinity of the samples the data were imported in Origin™ and analyzed with the curve fitting module. The SAXS curves were converted into Kratky plots. The long periods of the lamellar domains were determined by the q values of the reflection maxima.
Exp. no. | Catalyst | GL/Cat | T (°C) | t (h) | T m (°C). | ΔHm (J g−1) |
---|---|---|---|---|---|---|
1 | DMAP | 200/1 | 180 | 0.5 | 221.3 | 103 |
2 | DMAP | 200//1 | 150 | 0.5 | 222.6 | 109 |
3 | DMAP | 200/1 | 120 | 24 | 191.6 | 36 |
5 | 1,2-DMI | 200/1 | 120 | 24 | — | — |
6 | TPP | 200/1 | 150 | 3 | — | — |
7 | TPP | 200/1 | 120 | 3 | — | — |
8 | TPP | 100/1 | 120 | 3 | — | — |
The mass spectrum exclusively exhibited peaks of cPGAs in the low molar mass range (Fig. 1). Especially remarkable is the mass distribution of the cycles, because even-numbered cycles are largely predominant over the full mass range. Such a mass spectrum was not observed in previous studies.41–44 This finding suggests that the propagation rate may have exceeded that of the transesterification reaction, a notable observation given the elevated temperature and the results obtained with pyridine (see below).
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Fig. 1 MALDI TOF mass spectrum of cPGA prepared with DMAP in bulk at 150 °C (no. 2, Table 1). |
Complete conversion at 180 or 150 °C entailed one melting endotherm in the DSC heating trace with a minimum around 222 °C (Fig. 2A). This value was also found for other cyclic PGAs. At 120 °C, the conversion with DMAP was incomplete, even after 24 hours, as demonstrated by a broad melting endotherm of unreacted glycolide, ranging from 50 to 90 °C, in the DSC heating trace (Fig. 2B), as well as a strong melting endotherm of polyglycolide (Fig. 2B).
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Fig. 2 DSC heating traces (1st heating) of (A) cPGA prepared with DMAP at 150 °C (no. 2, Table 1), (B) prepared with TPP at 150 °C (no. 6, Table 1). |
An experiment with 1,2-DMI at 120 °C (no. 3, Table 1) produced a sample with nearly complete conversion after 24 hours. The mass spectrum displayed a predominance of cyclic PGAs below 3000 m/z; however, mass peaks of unidentified linear species dominated at higher masses, and the reaction product exhibited an almost black discoloration. Finally, three experiments with TPP as the catalyst were conducted. All three experiments had the following features in common: the mass peaks of cyclic PGAs dominated the mass range up to m/z 5000 but were accompanied by mass peaks of at least three types of linear species. Furthermore, despite the relatively rapid solidification of the reaction mixture, conversions were apparently all below 50%, as indicated by a melting endotherm of glycolide in the DSC heating traces, even at 150 °C (in analogy to Fig. 2B). TNPP experiments were conducted at 120 °C, 150 °C, and 180 °C; however, all three experiments failed to yield PGA. In summary, this first series of experiments revealed that GL can be polymerized via a zwitterionic mechanism even at temperatures as low as 120 °C, but tertiary amines are needed as catalysts. However, due to the intense side reactions and strong discoloration, DMAP and 1,2-DMI were not promising catalysts for preparative purposes.
Exp. no. | GL/Py | T (°C) | t (h) | Yield (%) | M n | M w |
---|---|---|---|---|---|---|
a Chlorobenzene was added in a 1/1 (v/v) ratio relative to pyridine. | ||||||
1 | 1//4 | 120 | 2 | 92 | 1350 | 2100 |
2 | 1/1 | 120 | 2 | 95 | 1400 | 2250 |
3A | 10/1 | 120 | 2 | 91 | 1320 | 2300 |
3B | 10/1 | 120 | 24 | 94 | 1350 | 2400 |
4A | 20/1 | 120 | 2 | 92 | 1400 | 2450 |
4B | 20/1 | 120 | 24 | 94 | 1450 | 2700 |
5A | 40/1 | 120 | 2 | 93 | 1600 | 3100 |
5B | 40/1 | 120 | 24 | 95 | 1750 | 3750 |
6 | 100/1 | 120 | 24 | 93 | 1850 | 3600 |
7 | 200/1 | 120 | 24 | 96 | 1800 | 3600 |
8 | 400/1 | 120 | 24 | Low conv. | — | — |
9 | 1/1 | 100 | 24 | 92 | 1450 | 2200 |
10 | 1/1 | 80 | 24 | 65 | 1400 | 2200 |
11a | 1/1 | 80 | 24 | 29 | 1450 | 2700 |
12 | 1/2 | 60 | 24 | 11 | — | — |
Three more experiments were conducted at lower temperatures with a GL/Py ratio of 1:
1 (no. 9–11, Table 2). At 100 °C, the initially clear solution turned cloudy after approximately one hour, and PGA began to crystallize on the glass walls of the reaction vessel. The same phenomenon was observed at 80 °C after two hours. After 22 hours, the resulting PGAs were isolated as crystalline powders. Most PGAs prepared with pyridine were soluble in HFiP, and GPC measurements yielded extremely low molecular weights in all cases.
Two noteworthy trends emerged. First, the molecular weights increased slightly with increasing monomer concentration. Second, most elution curves were bimodal, as illustrated in Fig. 3, or in a few cases even trimodal (Fig. S1 and S2, SI). Surprisingly, the dispersities were rather low, mainly ranging from 1.25 to 1.40, despite the bimodality of the GPC curves. The low molecular weights have two advantages. First, the MALDI TOF mass spectra are representative of most of the components in the PG samples. Second, the low molecular weights indicate that pyridine-catalyzed polymerization is a complementary approach to polymerizations catalyzed with tin compounds, which yield extremely high molecular weight PGAs.41,42 Such low molecular weights are, of course, useless for any mechanical application, but may be of interest for 3D printing of biodegradable medical devices by photopolymerization45 or in academic studies such as crystallization kinetics.
The mass spectra of all samples exclusively displayed peaks of cycles and most spectra were quite similar to that of Fig. 4A However, the PGAs prepared at 100 °C or below displayed a predominance of the even-numbered cycles over the odd-numbered ones quite analogous to the spectrum of Fig. 1 (and Fig. S3, S4). Unfortunately, the signal-to-noise (S/N) ratios of these mass spectra were poor compared to those of polylactide. The poor performance of PGA in MALDI TOF mass spectrometry results from the strong interchain forces between the densely packed PGA chains, a phenomenon that has also been observed in previous studies based on other catalysts.41–44
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Fig. 4 MALDI-TOF mass spectra of cPGAs prepared with pyridine at 120 °C (A) no. 3, Table 2, (B) after annealing with SnOct2 at 140 °C for 1 h (no. 1A, Table 4). |
Since all cyclic PGA samples prepared with pyridine exhibited a reddish or brownish discoloration that appeared to be inherent to the liquid phase, two attempts were made to remove the discoloration. The first attempt involved extracting the color using refluxing anhydrous dichloromethane or toluene. However, this method was not very successful because it was difficult to obtain the PGAs from experiments No. 1 and 2 (Table 2) as fine powders. Another attempt to purify the PGAs involved dissolution in HFiP, followed by precipitation in a 50/50 (v/v) mixture of THF and toluene. This method yielded PGA in the form of an ochre or grayish powder. The color and intensity of the discoloration decreased with the temperature. The PGA isolated from the 80 °C experiment had an ochre color and the PGA obtained at 60 °C showed a yellowish discoloration. The discoloration is most likely due to side reactions initiated by deprotonation (Scheme 3). This hypothesis is supported by the following observations. Deep red discoloration was also observed when L-lactide was heated in refluxing pyridine. After 24 hours, no polymerization was detectable, but the lactide was largely racemized, as indicated by a broad melting endotherm between 25 and 35 °C (after complete evaporation of the pyridine in vacuo), which is typical of contaminated meso-lactide (L-lactide has a Tm of 98–99 °C, and rac-D,L-lactide has a Tm of 125–126 °C). Furthermore, a reddish/brownish discoloration appears rapidly when a trialkyl amine is added to an aliphatic acid chloride solution with a proton in the α-position. Since H. Staudinger's work, it has been known that this reaction yields ketenes by dehydrohalogenation. The ketenes, which can also be formed from glycolide (see Scheme 4), cause a variety of side reactions. Considering the risk of deprotonation and subsequent side reactions, the low basicity of pyridine is advantageous compared to the more basic amines used in this study.
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Fig. 5 Schematic illustration of (A): an extended-ring crystallite made up by cycles of nearly identical ring size, (B) a crystallite formed by once-folded cycles. |
The HFiP was evaporated, and the crystallized residue was annealed at 140 °C for one or six hours (Table 4). Regardless of the time, the mass spectra of both samples displayed the STP known from cPGAs prepared at high temperatures in bulk (Fig. 4B).41–44 Characteristic for the STP of annealed cPGAs is the preferential formation of cycles with DP values of 20, 24, 28, 32, and 36 GA units. The reason, why these ring sizes represent a thermodynamic optimum remains unclear at this time. However, these experiments confirm the authors’ previous hypothesis.
In addition to the STP, the mass spectrum obtained after annealing with SnOct2 displayed another interesting phenomenon. Linear byproducts were formed, and these linear PGAs exhibited a mass distribution that corresponded to the most probable distribution initially calculated by Flory.46 The finding that STP cycles and linear chains had two different mass distributions indicates that they form separate crystallites. This phenomenon was quite recently also observed for alcohol-initiated and SnOct2-catalyzed ROPs of GL43 and it was found for the simultaneous formation of cyclic and linear PLAs.47,48
Finally, it should be noted that considering Fig. 1 and 4, the mass spectra presented in this work display three different distribution patterns. In previous publications only the pattern of Fig. 4B was observed.41–44
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Fig. 6 DSC heating traces (1st heating) of cPGA prepared with pyridine at 120 °C: (A) GL/Py = 1/4, (no. 2, Table 2), (B) GL/Py = 1/10 (no. 1, Table 2). |
Exp. No. | GL/Py | T (°C) | T m (°C). | ΔHm (J g−1) | Cryst.![]() |
L (nm) |
l
c![]() |
---|---|---|---|---|---|---|---|
a Calculated with a ΔHm0 of 206 J g−1. b Calculated from L by multiplication with the crystallinity. | |||||||
1 | 1/1 | 120 | 219.5 | 105 | 51 | 6.9 | 3.4 |
2 | 1//4 | 120 | 210.1 | 119 | 58 | 7.3 | 3.6 |
4 | 1/1 | 100 | 120.0 | 104 | 50 | 7.5 | 3.7 |
5 | 1/1 | 80 | 220.2 | 107 | 52 | 6.8 | 3.4 |
6 | 1/2 | 60 | 215.4 | 148 | 71 | 6.3 | 3.1 |
7 | 10/1 | 120 | 217.3 | 118.6 | 57 | 7.3 | 3.6 |
8 | 20/1 | 120 | 219.0 | 110.6 | 53 | — | — |
9 | 100/1 | 120 | 221.5 | 97.8 | 45 | — | — |
10 | 200/1 | 120 | 216.7 | 65.3 | 32 | — | — |
Regardless of topology or synthetic method, it is characteristic for PGA that the L-values are below 8 nm and the thickness of the crystallites (lc) is low (typically <4 nm), much lower than in the case of PLA.47,48 The long-distance values (L) measured for the cPGAs prepared with pyridine agree with this trend, as demonstrated by the L- and lc-values listed in Tables 3 and 4. These samples are characterized by relatively broad and weak reflections, which suggest small crystallites and a low degree of crystallinity (in agreement with the DSC measurements), as illustrated by curve A in Fig. 7. Upon annealing at 140 °C, the first- and second-order reflections sharpened, indicating an improvement in the third-order within the spherulites (Fig. 7(B)).
The lc values found for the cPGAs fit in with a sequence of 10–13 glycolyl units, sine the length of 10 repeat units amounts to 3.0 nm.49 These degrees of polymerization (DPs) correspond, in turn, to ring sizes of 20–26 repeat units Since lc values listed in Tables 3 and 4 only represent a rough estimation and since the thickness of the crystallites may cover a broad distribution, it is plausible that also slightly larger cycles having DPs up to 30 or32 may form extended-ring crystallites, whereas larger cycles have to fold at least once to fit in with a crystal thickness around 31–37 nm.
However, folding considerably reduces the perfection of the crystallites in two ways as illustrated in Fig. 5B. First, insufficient length of a folded ring may cause defects inside crystal lattice. Second, the surface has a lower degree of order, because the loops resulting from folding adopt an orientation perpendicular to the loops formally representing ring end groups. As mentioned above, the perfection of extended-ring crystallites has the consequence that they crystalize separately from linear chains. This phenomenon raises now the question, if extended-ring crystals also strictly exclude folded rings, so that cycles folding one or twice upon crystallization form separate crystallites. A detailed study of this problem was beyond the scope of this work and it will be difficult any way to find an analytical method allowing for solution of this problem. Nonetheless, this discussion illustrates, why low molar mass cyclic PGAs and PLAs are interesting substrates for studies of crystallization phenomena.
Fig. S1 GPC elution curves of the PGAs No. 3A and 4A, Table 2. Fig. S2 GPC elution curve of PGA No. 7, Table 2. Fig. S3 MALDI TOF mass spectrum of PGA No. 9, Table 2. Fig. S4 MALDI TOF mass spectrum of PGA No. 11, Table 2. See DOI: https://doi.org/10.1039/d5py00762c.
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