Hans R. Kricheldorf*a,
Steffen M. Weidnerb and
Andreas Meyerc
aInstitut für Technische und Makromolekulare Chemie der Universität Hamburg, Bundesstr. 45, D-20146 Hamburg, Germany. E-mail: kricheld@chemie.uni-hamburg.de
bBAM, Bundesanstalt für Materialforschung und -prüfung, Richard Willstätter Straße 11, 12489 Berlin, Germany
cInstitut für Physikalische Chemie der Universität Hamburg, Grindelallee 117, D-20147 Hamburg, Germany
First published on 14th April 2021
Alcohol-initiated ROPs of L-lactide were performed in bulk at 160 °C for 72 h with variation of the catalyst or with variation of the initiator (aliphatic alcohols). Spontaneous crystallization was only observed when cyclic Sn(II) compounds were used as a catalyst. Regardless of initiator, high melting crystallites with melting temperatures (Tm) of 189–193 °C were obtained in almost all experiments with Sn(II) 2,2′-dioxybiphenyl (SnBiph) as catalyst, even when the time was shortened to 24 h. These HTm poly(lactide)s represent the thermodynamically most stable form of poly(L-lactide). Regardless of the reaction conditions, such high melting crystallites were never obtained when Sn(II) 2-ethylhexanoate (SnOct2) was used as catalyst. SAXS measurements evidenced that formation of HTm poly(L-lactide) involves growth of the crystallite thickness, but chemical modification of the crystallite surface (smoothing) seems to be of greater importance. A hypothesis, why the “surface smoothing” is more effective for crystallites of linear chains than for crystallites composed of cycles is discussed.
Quite recently, the authors have reported that neat SnOct2 produces cyclic polylactides and not as believed for several decades' linear ones.11 Hence, it is highly likely that the Pennings group had cyclic polylactide in hand and observed properties influenced by transesterification reactions catalyzed by SnOct2.
In this context, it was the purpose of this work to find conditions allowing for the preparation of high Tm linear pol(L-lactide)s initiated by alcohols (or primary amines), and to find an explanation why alcohol-initiated ROPs and polymerization mechanisms yielding preferentially cyclic polylactides behave quite differently with regard to formation of HTm crystallites. Structures and labels of the catalysts used and/or discussed in this work were compiled in Scheme 1.
Annealing experiments with preformed poly(L-lactide) ethyl esters (Table 6).
A portion of 5.76 g (80 mmol of lactyl units) was dissolved in dry dichloromethane (50 mL) and a catalyst (0.04 mmol of SnOct2, DSTL or BuSnNaph) was added. The resulting solution was evaporated under normal pressure with slow heating up to 120 °C whereupon the polylactide crystallized.
The GPC measurements were performed in a modular system kept at 40 °C consisting of an isocratic pump, 1 mL min−1 and a refractive index detector (RI-501-Shodex). Samples were manually injected (100 μL, 2–4 mg mL−1). For instrument control and data calculation Clarity software (GPC extension, DataApex) was used. The calibration was performed using polystyrene standard sets (Polymer Standards Service – PSS, Mainz). All molecular weights listed in Tables 1–3 and 5 are uncorrected. They overestimate the real molecular weights by approximately 50% corresponding to a correction factor of 0.67 (±0.01).
The DSC heating traces were recorded on a (freshly with indium and zinc 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 considered. The crystallinities were calculated with a maximum melting enthalpy of −106 J g−1
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. The sample-detector distance for SAXS was 1.6 m. For WAXS, a distance of 0.1 m was used, allowing us to detect an angular range of 2Θ = 5°–33°. The patterns were recorded with a Rayonix™ SX165 CCD-Detector and the accumulation time per SAXS measurement was 1200 s and for WAXS 300 s.
DPDAK, a customizable software for reduction and analysis of X-ray scattering data sets was used for gathering 1D scattering curves.16 For the evaluation of the crystallinity of the samples the data were imported in Origin™ and analyzed with the curve fitting module. After subtracting of the instrumental background, the integral intensity of the crystalline reflections was divided by the overall integral intensity to determine the crystallinity xc.
Exp. no. | Catalyst | Spherulitesa (%) | Mn | Mw | Tm (°C) | ΔHm (J g−1) |
---|---|---|---|---|---|---|
a Estimated volume fraction of the reaction mixture.b Almost completely crystallized.c With another batch of L-lactide only 50–60 vol% of the reaction mixture had crystallized. | ||||||
1 | DSTL | 0 | — | — | — | — |
2 | DSTD | ∼5–10 | — | — | — | — |
3 | BuSnBuca | 0 | — | — | — | — |
4 | BuSnCyca | 0 | — | — | — | — |
5 | BuSnBiph | 0 | — | — | — | — |
6 | BuSnNaph | ∼20–25 | — | — | — | — |
8 | SnBuca | ∼60–80 | — | — | — | — |
10 | SnBiph | 80–95 | 18500 | 40000 | 193.0 | 87 |
11 | SnNaphb,c | 80–95 | 16000 | 38000 | 178.0 | 65 |
On the basis of these results (Table 1), a series of ROPs was performed with SnBiph as catalyst and variation of the initiator (Table 2). This second series of polymerizations had the purpose to find out if and to what extent the initiator influences the formation of HTm crystallites. The steric demands of the initiator were varied over a broad range, but crystallization was observed for all initiators (Table 2) and all experiments yielded polylactides having Tm's > 189 °C. However, the first experiment with EtLac at a Lac/In ratio of 100/1 did not crystallize although the parallel experiment with a Lac/In ratio of 300/1 had crystallized (No. 2). For experiment 1A the EtLac was added in the form of a 2 M solution in toluene and when the experiment was repeated (No. 1B) with addition of neat EtLac complete crystallization was achieved. A similar observation was made for initiation with n-butanol. The first experiment failed to crystallize, whereas the second polymerization yielded a completely crystallized polylactide. These observations suggest that a lack of crystallization may in individual cases result from slow or hindered nucleation. Therefore, several experiments of Table 1 were repeated to check, if the failure of crystallization was reproducible and it was found to be reproducible. At this point, it should also be mentioned that the SEC data listed in Table 2 evidence a rough dependence of the molecular weights on the Lac/In ratio. A more precise control of the molecular weights may not be expected because of transesterification reactions including formation of cycles. In summary, the results obtained from the experiments of Table 2 underline the extraordinary usefulness of SnBiph and confirm that with an optimum catalyst linear HTm polylactides can be prepared via alcohol initiated ROPs. After this success, those experiments based on a Lac/In ratio of 200/1 were repeated with a time of 1 d for the following reasons:
Exp. no. | Initiator | Lac/In | Mn | Mw | Tm (°C) | ΔHm (J g−1) | Cryst. (%) | L (nm) | lc (nm) |
---|---|---|---|---|---|---|---|---|---|
a Ethyl lactate was added as 2 M solution in toluene.b Neat ethyl lactate was added.c 10-Undecenol.d 2-hydroxymethyl naphthalene.e 1,12-Dodecane diol. | |||||||||
1Aa | EtLac | 100/1 | No cryst. | — | — | — | — | — | — |
1Bb | EtLac | 100/1 | 13500 | 27500 | 192.5 | 84.0 | 80 | 28 | 23 |
2 | EtLac | 300/1 | 37500 | 77000 | 195.5 | 83.5 | 79 | 30 | 24 |
3 | n-Butanol | 200/1 | No cryst. | — | — | — | — | — | — |
4 | 10-Undc | 100/1 | 20000 | 42000 | 190.5 | 84.5 | 80 | 25 | 20 |
5 | 10-Undc | 200/1 | 30000 | 64000 | 192.3 | 83.5 | 79 | 28 | 23 |
6 | 1-Hmnd | 100/1 | 19000 | 42500 | 188.5 | 87.0 | 82 | 26 | 21 |
7 | 1-Hmnc | 200/1 | 27000 | 66000 | 190.0 | 89.0 | 83 | 27 | 23 |
8 | 1,12-Dode | 200/1 | 29500 | 68500 | 190.2 | 84.0 | 77 | 30 | 23 |
9 | 1,12-Dode | 400/1 | 44000 | 92000 | 193.5 | 92.0 | 86 | 26 | 23 |
(1) A shorter time is more attractive from a preparative point of view and reduces the risk of partial racemization and other side reaction.
(2) It should be found out, if the longer time of three days has a significant influence on Tm and ΔHm.
(3) The results should be compared with those obtained from polymerizations catalyzed by SnOct2 (see Table 4 below).
All polymerizations stopped after 1 d yielded crystalline polylactides but only in three experiments a Tm of 190 °C or higher was achieved, whereas in the case of n-butanol and 1,12-dodecanediol the Tm's were as low as 184.0 and 183.5 °C (Table 3). Hence, these experiments demonstrate that at the shorter time the initiator has indeed an influence on the perfection of the resulting crystallites. However, a straightforward explanation based on the steric demands of the initiator proved impossible, because the volume of 10-undecenol, which gave a high Tm, is more than twice as high than that of n-butanol. These unexpected results like those of Table 1 justified, why it made sense to conduct numerous experiments with broad variation of all experimental parameters.
Exp. no. | Alcohol | Mn | Mw | Tm | ΔHm (J g−1) | Crystal (%) |
---|---|---|---|---|---|---|
1 | EtLac | 24500 | 45000 | 190.0 | 83.5 | 79 |
2 | n-BuOHl | 20000 | 43000 | 184.0 | 75.0 | 71 |
3 | 10-Und | 36500 | 80000 | 192.0 | 80.5 | 76 |
4 | 1-Hmn | 34500 | 71000 | 190.5 | 79.0 | 75 |
5 | Dod | 34000 | 61000 | 183.5 | 71.0 | 67 |
Exp. no. | Initiator | Lac/Cat | Lac/In | Spherulitesa (%) | Tm (°C) | ΔHm (J g−1) |
---|---|---|---|---|---|---|
a Estimated vol% of the reaction mixture.b These experiments were repeated and the failure to crystallize was reproduced. | ||||||
1 | EtLac | 100/1 | 1000/1 | 0 | — | — |
2b | EtLac | 200/1 | 1000/1 | 0 | — | — |
3 | Lac. amide | 200/1 | 1000/1 | 20–30 | — | — |
4 | n-Butanol | 100/1 | 1000/1 | 0 | — | — |
5b | n-Butanol | 200/1 | 1000/1 | 0 | — | — |
6 | 10-UND | 100/1 | 1000/1 | 0 | — | — |
7b | 10-UND | 200/1 | 1000/1 | c. 5 | — | — |
8 | 2-HMN | 100/1 | 500/1 | c. 50 | 184.0 | 69.0 |
9 | 2-HMN | 100/1 | 1000/1 | c. 60–70 | 187.5 | 79.5 |
10 | 2-HMN | 200/1 | 500/1 | c. 15 | — | — |
11 | 2-HMN | 200/1 | 1000/1 | c. 5 | — | — |
12 | BnOH | 100/1 | 1000/1 | 0 | — | — |
13 | BnNH2 | 100/1 | 1000/1 | 0 | — | — |
A first noteworthy result is the crystallization of the polylactides prepared with EtLac as initiator (No. 1 and 2, Table 3). Since Tm's < 180 °C were found, these results demonstrate the reproducibility of an experiment presented in ref. 8, which was conducted under exactly the same conditions as experiment No. 2 in Table 3 of this work. This point needs to be emphasized for two reasons. Firstly, it illustrates the conspicuous difference between the catalysts SnBiph and SnOct2. Secondly, it demonstrates together with the other results compiled in Table 4, that in the case of SnOct2 the initiator has a considerable influence on formation and perfection of the crystallites. With butanol and 10-undecenol no crystallization occurred, and this failure was reproducible. However, partial crystallization was again observable, when 2-hydroxymethyl naphthalene served as initiator and it was also found that a low Lac/In ratio was advantageous for the extent of crystallization. The most surprising result came up when the DSC measurements showed that Tm's of the polylactides from the 100/1 experiments (No. 6 and 7, Table 3) were as high as 184.0 and 187.5 °C. These Tm's were somewhere in between those of typical LTm and HTm crystallites and demonstrated for the first time that SnOct2 may produce crystallites with higher perfection than the normal LTm species, but the results of experiments No. 6 and 7 were still far from the optimum which was achieved with SnBiph under the same conditions. Nonetheless, these unexpected results prompted the authors to study the effect of two other aromatic initiators and since the highest Tm was obtained with 2-HMN at a Lac/In ratio of 100/1, the additional experiments with benzyl alcohol and benzyl amine (No. 12 and 13) were performed with this Lac/In ratio, but no crystallization was observed.
To complete the comparison of SnOct2 with SnBiph, two small series of polymerizations were performed with variation of the temperature (Table 5). All SnBiph-catalyzed polymerizations crystallized, but HTm crystallites with a Tm > 190 °C were only obtained at the highest temperature (160 °C). This result contrasts with SnBiph-catalyzed polymerization performed in the absence of an alcohol, because neat SnBiph yielded HTm polylactide even at 120 °C.8 This comparison demonstrates again that alcohol initiated ROPs are unfavourable for the formation of HTm crystallites. With SnOct2 no crystallization occurred at 160 °C and at lower polymerization temperatures the Tm's were all below 184 °C. In other words, the combination of SnOct2 with alcohol proved again to be particularly unfavourable for the formation of HTm crystallites.
Exp. no. | Catalyst | Temp. (°C) | Spherulites (vol%) | Mn | Mw | Tm (°C) | ΔHm (J g−1) | Cryst. | L (nm) | lc |
---|---|---|---|---|---|---|---|---|---|---|
1 | SnBiph | 160 | 90–100 | 30000 | 51000 | 191.5 | 84.0 | 79 | 28 | 22 |
2 | SnBiph | 150 | 90–100 | 29000 | 43500 | 188.5 | 88.0 | 83 | 21 | 18 |
3 | SnBiph | 140 | 90–100 | 29000 | 39000 | 187.0 | 87.0 | 82 | 20 | 16 |
4 | SnBiph | 130 | 90–100 | 26000 | 31700 | 182.5 | 87.5 | 83 | 19 | 15/16 |
5 | SnOct2 | 160 | — | — | — | — | — | — | — | — |
6 | SnOct2 | 150 | 30–40 | 19500 | 44700 | 183.5 | 80.5 | 76 | 18 | 14 |
7 | SnOct2 | 140 | 90–100 | 22000 | 35700 | 183.5 | 79.0 | 75 | 19 | 14 |
8 | SnOct2 | 130 | 90–100 | 21000 | 28300 | 179.5 | 78.5 | 74 | 17 | 12/13 |
All the results reported above suggested that a larger number of OH end groups on the surface of the lamellar crystal is unfavourable for the formation of HTm poly(L-lactide). As a hypothetical explanation of these results, it may be concluded that the OH groups reduce the mobility of the catalyst either by donor–acceptor interaction (coordination) with the tin atoms or by temporarily (reversible) formation of covalent bonds. This assumption is supported by the well-known mechanism of SnOct2/alcohol catalyzed polymerizations which includes as first step the reversible formation of Sn-alkoxide groups (Scheme 2, eqn (1) and (2)). This hypothesis also explains why crystallites consisting of cyclic polylactides are more prone to modification by transesterification on their surface. Its surface is exclusively covered with loops and thus, their ester groups are easily accessible to the catalysts. Furthermore, the ester groups in the loops are slightly more reactive than those in linear chain segments, due to energetically less favourable conformations (cisoid versus transoid). In order to shed more light on this phenomenon, the annealing experiments summarized in Table 6 were conducted.
Exp. no. | Substrate | Cat. used for annealing | T (°C) | t (h) | Tm (°C) | ΔHm (J g−1) | Cryst. (%) |
---|---|---|---|---|---|---|---|
a The EtLac-initiated, SnOct2-catalyzed product of exp. no. 8, Table 5, was used as substrate.b AA preformed poly(L-lactide) prepared with EtLac as initiator (Lac/In = 200/1) and SnOct2 as catalyst (Lac/Cat = 1000/1) was acetylated with acetic anhydride plus pyridine and used as substrate. | |||||||
1 | HO-PLA-Eta | SnOct2 | 160 | 48 | 180.5 | 92 | 86 |
2 | HO-PLA-Eta | SnOct2 | 170 | 24 | 184.0 | 77 | 72 |
3 | AcO-PLA-Etb | — | 160 | 48 | 180.0 | 84 | 79 |
4 | AcO-PLA-Etb | — | 170 | 24 | 180.5 | 80 | 75 |
5 | AcO-PLA-Etb | SnOct2 | 160 | 48 | 183.5 | 91 | 86 |
6 | AcO-PLA-Etb | SnOct2 | 170 | 24 | 184.5 | 87.5 | 82 |
7 | AcO-PLA-Etb | DSTL | 170 | 24 | 182.5 | 90.5 | 86 |
8 | AcO-PLA-Etb | BuSnNaph | 179 | 24 | 184.5 | 89.0 | 85 |
Fig. 1 DSC heating traces of polylactides prepared by ethyl L-lactate-initiated ROPs in bulk at 160 °C/3 d: (A) with SnBiph (No. 10, Table 1), (B) with DSTD (No. 2, Table 1). |
Fig. 2 DSC heating traces of a polyLA prepared with SnNaph as catalyst and ethyl L-lactate as initiator at 160 °C/3 d (No. 8, Table 1, see footnote c). |
Fig. 3 DSC heating traces of polyLA prepared with SnOct2 as catalyst and 1-HMN as initiator (LA/In = 100/1) at 160 °C, 3 d: (A) after 1 h (No. 9, Table 4), (B) after 0.5 h (No. 8, Table 4). |
When the sample picked up for the DSC measurements contained a large amount of amorphous phase, the glass-transition (around 50 °C) was clearly observable and followed by crystallization endotherm with a maximum around 105 °C (Fig. 2). The crystallites formed during this crystallization process had a low perfection and melted around 167 °C. The fourth feature was finally the melting endotherm of the HTm crystallites formed during the polymerization. DSC heating traces with a similar structure were also obtained from polylactides prepared with SnOct2 in the experiments of Table 5 (Fig. 3). Again, crystallization of the amorphous phase followed by a melting endotherm at low temperature (around 167 °C) can be seen. What is different from the DSC traces discussed before, is a strong endotherm at a temperature between 180 and 190 °C indicating a partial transformation of LTm into HTm crystallites.
Fig. 4 MALDI TOF mass spectra of ethyl lactate-initiated polylactides polymerized with (A) SnBiph at 150 °C/1 d (No. 2, Table 5), (B) SnOct2 at 140 °C/1 d (No. 7, Table 5). L = linear chains having ethyl ester end groups. |
However, when UND was used as initiator with a Lac/In ratio of 100/1 cycles were also absent after 3 d at 160 °C (Fig. 5A). Yet, at Lac/In ratio of 200/1 small amounts of cycles were formed as demonstrated in Fig. 5B. This difference agrees with results of a previous study which showed that back-biting is favors by lower In/Cat ratios corresponding to higher Lac/In ratios at constant catalyst concentration. However, with other alcohols cycles were also formed at Lac/Cat ratios of 100/1 as demonstrated in Fig. S1A (see ESI).†
Fig. 5 MALDI TOF mass spectra of polylactides initiated with 11-undecenol and catalyzed with SnBiph at 160 °C: (A) LA/In = 100/1, No. 4 Table 2, (B) LA/In = 200/1, No. 5, Table 2. L = linear chains having undecenyl ester end groups. |
The most interesting and somewhat surprising result was the existence of a maximum in the molecular weight distribution (MWD) between m/z 5000 and 6000, whenever semi-crystalline polylactides were measured (Fig. 4, 5, S1 and S2†). In principle, one may expect that a fully equilibrated polymer possesses a “most probable” distribution according to eqn (1) as first demonstrated by Flory for irreversible and reversible polycondensations.22
nx = p(x−1)(1 − p) | (1) |
Fig. 6 MALDI TOF mass spectrum of a polylactides prepared with Ph2SnCl2 as catalyst in bulk at 160 °C/1 h (reproduced from ref. 23). |
The most probable MWD results from an optimization of the entropy. Hence, it is obvious that the maxima observed in mass spectra of the semi-crystalline poly(L-lactide)s result from a gain in enthalpy, and the only source of a negative enthalpy change is in this system formation of more and more perfect crystallites. In other words, these maxima of the MWD suggest that a certain chain length is for thermodynamic reasons particularly prone to crystallize. Their “extraction” from the amorphous phase into the crystallites has the consequence that such chains are regenerated from the pool of shorter and longer chains by transesterification. Such a scenario was also observed, when cyclic polylactides were annealed at 120 °C for 15 d with a large amount of DSTL (Lac/Cat = 200/1).25 It was concluded that enthalpy-driven formation of new maxima in the MWD is characteristic for cyclic polylactides. The results presented in this study clearly prove that not the topology, but the chain length is decisive. A more detailed study and explanation of this phenomenon was outside the scope of this work.
In the previous study27 dealing with HTm crystallites of predominantly cyclic poly(L-lactide)s, it was found by means of SAXS measurements that the HTm polylactides possess lamellar crystallites with a greater thickness (lc values), than the standard LTm crystallites. Whereas lc-values in the range of 25–35 nm were typical for HTm crystallites, lc values in the range of 8–11 nm were found for the LTm counterparts. Hence, it was of interest, if this trend could be confirmed by the alcohol-initiated polylactides prepared in this work. For the first SAXS measurements, samples listed in Table 2 were selected, because for these samples the highest degree of perfection was expected. The lc-values listed in the last column of that table corresponded indeed to distances in the range of 21–25 nm (Fig. S4†), corresponding to a thickness growth by a factor of 2.0–2.2 relative to the usual thickness of LTm crystallites. However, a factor of 2.5–3.5 was found for most polymerization and annealing experiments in previous studies based on cyclic polyLAs.27
Another series of experiments which was particular interesting for SAXS measurements was the variation of the polymerization temperature illustrated in Table 5. As expected, form the relatively high Tm, the lc-value of 22 nm found for sample No. 1 (Fig. 7B) was in agreement with the formation of HTm crystallites. Furthermore, the other extreme, namely the LTm sample No. 8, prepared with SnOct2 at 130 °C was again in agreement with the expected trend: low Tm combined with a rather low lc-value (12–13 nm; Fig. 7A). The other measurements listed in Table 5 gave Tm and lc values in between these extremes.
Fig. 7 SAXS Kratky plots of polylactides prepared with ethyl lactate as initiator and with: (A) SnOct2 as catalyst at 130 °C (No. 8, Table 5), (B) SnBiph as catalyst at 160 °C (No. 1, Table 5), 1st o. = reflection of first order of lamellar long period L. |
In this connection, the most interesting result of this work is the finding that Tm's > 191 °C were achieved with a rather moderate increase of the lamellar thickness when the crystallites are formed by linear chains compared with crystallites composed of cyclic polyLA. This means that another factor played an important role, namely a considerable reduction of the surface free energy σe. According to the Gibbs–Thomson – eqn (2), a high Tm may be a consequence of a low σe or a high lc value. At identical Tm a lower crystal thickness as observed for the linear polyLAs of this work is therefore, correlated with a rather low surface free energy.
Tm= Tm0[1 − (2σe/r × ΔHm0 × lc)] | (2) |
Hence, the results of this work indicate that the alcohol-initiated linear chains are less favorable for the thickness growth of the crystallites than predominantly cyclic polylactides, but more favorable for a “smoothing” of the surface via transesterification. The transesterification reactions responsible for such a “smoothing” have been discussed in two previous publications, and thus should not be repeated here again. The demonstration that chemical “smoothing” of the crystallite surface plays an important role for the rise of Tm is remarkable for two reasons. First, to the best knowledge of the authors this phenomenon has never been documented before. Second, an explanation is required why the chemical smoothing is more effective when crystallites of linear chains are involved relative to crystallites composed of cyclic polyLAs. Illustrated in Fig. 8A, the surface of crystallites composed of cycles is exclusively covered by loops, which include energetically unfavorable conformations of the repeat units. Due to the steric demands of these loops, directly neighboring loops cannot have the same size. However, in the case of crystallites based on linear chains, loops may be neighbored by sterically less demanding and more flexible linear chain ends (Fig. 8B). Hence, smoothing by transesterification may create a more homogeneous surface with a smaller thickness of the rigid amorphous fraction (RAF), whereas the surface of crystals formed by cycles remains rougher and includes a higher level of conformational energy.
Fig. 8 Hypothetical illustration of the smoothed surface of crystallites consisting of cyclic polyLA (A) or of linear polyLA (B). |
Finally, it should be mentioned that the SAXS patterns of all samples having Tm's around 184 °C or higher show a second order refection (Fig. 7 and S4†), which indicates a rather high 3-dimensional order of the crystallites in the spherulites. Fig. 9 presents a schematic summary and illustration of the consequences that transesterification reactions in the mobile and immobile disordered phase have on shape and 3-dimensional ordering of the crystallites.
Fig. 9 Schematic illustration of the morphological change caused by transesterification reactions across the rigid amorphous phase on the large surfaces of the lamellar crystallites. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra01990b |
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