Open Access Article
Xin
Zhang
,
Timothy J.
Prior
and
Carl
Redshaw
*
Plastics Collaboratory, Department of Chemistry, The University of Hull, Cottingham Rd, Hull HU6 7RX, UK. E-mail: c.redshaw@hull.ac.uk
First published on 1st July 2022
Reaction of benzilic acid, Ph2C(OH)(CO2H), L1H2, with equimolar amounts of M(OR)5 (M = Nb, Ta) led, following work-up, to the tetranuclear complexes [Nb4(OEt)8(L1)4(μ-O)2] (1) or [Ta4(OEt)8(L1)4(μ-O)2]·0.5MeCN (2·0.5MeCN), respectively. Similar use of 2,2′-diphenylglycine, Ph2C(NH2)(CO2H), L2H3, led to the isolation of the dinuclear complexes [Nb2(OEt)4(L2H2)4(μ-O)]·2MeCN (3·2MeCN) or [Ta2(OEt)4(L2H2)4(μ-O)]·2.25MeCN (4·2.25MeCN). The molecular structures of 1–4 are reported. Complexes 1–4 have been screened for their potential to act as catalysts for the ring opening polymerization (ROP) of ε-caprolactone (ε-CL) and rac-lactide (r-LA), with or without benzyl alcohol (BnOH) present. In the case of ε-CL, complex 1 displayed best activity with >99% conversion at 100 °C, whilst 3 and 4 were virtually inactive under the same conditions. All complexes show moderate activities towards the ROP of r-LA at 160 °C, with 1–3 producing heterotactic enriched PLA while 4 afforded isotactic enriched PLA. Copolymerization studies revealed the most efficient system involved the initial addition of r-LA (for 6 h) followed by ε-CL (for 42 h), which led to 99% conversion for each of the monomers. Block copolymers of PLA-b-CL and PCL-b-LA and random copolymers PLA-co-CL were successfully synthesized by adjusting the feed sequence.
O character. There is minor disorder in the orientation of the ethoxide alkyl chains, but this was readily modelled using standard procedures.
The space group symmetry assembles pairs of these units into tetranuclear molecules that are non-centrosymmetric and contain four niobium atoms, four benz2−, eight ethoxide ligands and two μ2-oxide anions bridging between pairs of niobium atoms.
Similar use of [Ta(OEt)5] led to the isolation of the complex [Ta4(OEt)8(L1)4(μ-O)2]·0.5MeCN (2·0.5MeCN). Crystals suitable for an X-ray diffraction study were grown from a saturated solution of acetonitrile at ambient temperature. The molecular structure is shown in Fig. 2, with selected bond lengths and angles given in the caption; for an alternative view see Fig. S2, ESI.† This is isostructural with the Nb compound and differs only in the presence of a small amount of uncoordinated solvent that was modelled using a solvent mask (Squeeze) in Olex2.
The 1H NMR spectrum is consistent with the formulation with peaks assigned to aromatic protons (20H), as well as methylene (8H) and methyl (12H) groups of the ethoxide ligands, respectively. The IR spectra do not contain a sharp band at 3394 cm−1 corresponding to the ν(OH) stretching vibration of the parent L2H2 acid. The presence of new peaks at 486, 462 cm−1 suggest the formation of M–O bonds (Fig. S3, ESI†). In the mass spectrum of 1, peaks at m/z 1487.40 corresponds to loss of four OEt and H+ from the parent ion (Fig. S4, ESI†); the ESI-MS of 2·0.5MeCN is shown in Fig. S5, ESI.†
There is minor disorder in the ethoxide and also the orientation of the phenyl groups. This was dealt with satisfactorily using standard techniques within Olex2. A small amount of unbound solvent was modelled using a solvent mask (Squeeze) within Olex2.
Similar use of [Ta(OEt)5] led to the isolation of the complex [Ta2(OEt)4(L2H2)4(μ-O)]·2.25MeCN (4·2.25MeCN). Crystals suitable for an X-ray diffraction study were grown from a saturated solution of acetonitrile at ambient temperature. The molecular structure is shown in Fig. 4, with selected bond lengths and angles given in the caption; for an alternative view see Fig. S7, ESI.† The Ta compound is isostructural to 3 and differs only in the amount of solvent present.
The 1H NMR spectrum supports the formulation of 3·2MeCN and 4·2.25MeCN with the multiple aromatics peaks between 7.03–7.75 ppm, and quartets at 3.50–2.52 ppm and a triplet at 1.06–1.10 ppm assigned to the ethoxide groups; the signal for the NH2 groups appear as a broad peak at ca. 2.2 ppm. In the IR spectrum of the parent acid L2H3, there are two absorptions near 3441 and 3267 cm−1 (assigned to symmetric and asymmetric ν(N–H) stretching), and two weak ν(N–H) absorptions are found at near 3440 and 3314 cm−1 for complexes 3·2MeCN and 4·2.25MeCN (Fig. S8, ESI†). In the mass spectrum of complex 3·2MeCN, the peaks at m/z 1366 corresponds to loss of 3H+ from the parent ion (Fig. S9, ESI†); the ESI-MS of 4·2.25MeCN is given in Fig. S10, ESI.†
| Run | Cat. | [CL]0 : [cat]0 : [BnOH]a |
Conv.b (%) | M n (calc.) | M n (obs.) | PDId |
|---|---|---|---|---|---|---|
| a [CL] = 10.00 mmol, [catalyst 1 or 2] = 0.01 mmol, [3 or 4] = 0.02 mmol, [BnOH] = 0.04 mmol (0.01 M in toluene), 100 °C, 24 h. b Determined by 1H NMR spectroscopy. c M n(calc.) = 114.14 × [CL]0/[Nb/Ta]0 × conv.% + MBnOH, assuming one propagation chain per metal atom. d M n(obs) and PDI obtained by GPC in THF relative to polystyrene standards corrected by the Mark–Houwink correction factor Mn(obs) = MnGPC raw data × 0.56. e Run 9, the reaction was happened at 160 °C. | ||||||
| 1 | 1 | 250 : 1 : 1 |
>99 | 7170 | 12 000 |
1.2 |
| 2 | 2 | 250 : 1 : 1 |
50 | 3675 | 9000 | 1.9 |
| 3 | 3 | 250 : 1 : 1 |
2 | — | — | — |
| 4 | 4 | 250 : 1 : 1 |
2 | — | — | — |
| 5 | 1 | 250 : 1 : 0 |
76 | 5468 | 9000 | 1.2 |
| 6 | 2 | 250 : 1 : 0 |
38 | 2757 | 6000 | 1.3 |
| 7 | 3 | 250 : 1 : 0 |
1 | — | — | — |
| 8 | 4 | 250 : 1 : 0 |
1 | — | — | — |
| 9 | 4 | 250 : 1 : 0 |
87 | 12 459 |
10 000 |
1.3 |
| 10 | 1 | 125 : 1 : 1 |
99 | 3639 | 7000 | 1.4 |
| 11 | 1 | 500 : 1 : 1 |
91 | 13 091 |
28 000 |
1.3 |
| 12 | 1 | 1000 : 1 : 1 |
20 | 5815 | 9000 | 1.4 |
Complex 1 afforded PCL with high molecular weight (Mn = 12
000) and narrow molecular distribution (1.2) (Table 1, entry 1). When conducting the polymerizations in the absence of BnOH, the polymerization activity and molecular weight decreased slightly (Table 1, entries 5–8). When the mole ratio CL
:
Nb was increased from 125 to 500, the molecular weight increased from 7000–28
000 (PDI = 1.2–1.4) with the conversion rates and distributions remaining stable. Increasing the ratio to 1000
:
1 proved to be detrimental to the conversion rate (Table 1, entry 12).
A kinetics study for the polymerization of ε-CL using 1 and 2·0.5MeCN in the ratio [CL]0
:
[Nb/Ta]0
:
[BnOH] 250
:
1
:
1 at 100 °C was performed (Fig. 5). From the plot, there is an induction period (ca. 60 min.) for 1. The calculated slope of the linear section of the curve is equal to the apparent polymerization rate constant.24
For complex 2·0.5MeCN, there is a first-order dependence of the rate of the polymerization without any induction period. The rate constants (Kobs) are 250 × 10−4 min−1, R = 0.990 and 4.58 × 10−4 min−1, R = 0.999 for 1 and 2·0.5MeCN, respectively. From the rate constants, it is inferred that the polymerization rate is significantly faster for the Nb complex versus the Ta complex. In previous work,20 we have utilized tetraphenolate niobium and tantalum complexes for the ROP of ε-CL. Under the same conditions, such niobium complexes exhibited excellent conversions and afforded higher molecular weight products compared with the analogous tantalum complexes.
In the MALDI-TOF spectrum (Fig. 6), the PCL formed by 1 exhibits two major families of peaks. The main peaks are assigned to polymer chains with PhCH2O– end groups which agreed with the 1H NMR spectra (Fig. S12, ESI†). The results suggested the formation of Nb-OCH2Ph species acted as the initiator for the ROP via the coordination–insertion mechanism;25 signals at 7.34 and 5.10 ppm indicating a benzyl group and the peak at 3.64 ppm was ascribed to an OH terminal group. A second distribution of peaks is associated with ethoxy (–OCH2CH3) and hydroxyl (–OH) end groups, which could also be observed in the 1H NMR spectra (Fig. S12, ESI†). This result indicated that an ethoxide niobium complex was also present and involved in the ROP process via a coordination–insertion mechanism.26,27 The successive series showed that there was a m/z difference of 114 between neighbouring peaks, which corresponds to the molecular weight of the monomer. The end group of PCL isolated using 1 in the absence of BnOH was also investigated by MALDI-TOF, and the spectrum (Fig. S13, ESI†) confirmed that PCL with an ethoxy and hydroxyl (–OH) end groups was formed.
![]() | ||
| Fig. 6 MALDI-TOF spectrum of the PCL catalysed by complexes 1 (Table 1, entry 1); n is the degree of polymerization. | ||
:
[Nb/Ta]0
:
[BnOH] ratio 250
:
1
:
1 over 24 h. The results are depicted in Table 2. The reaction temperature was first investigated, and it was observed that when the temperature was 130 °C, only the L1H2 derived complexes 1 and 2·0.5 MeCN were active towards the ROP of r-LA, and the monomer conversion reached 40% after 24 h for 1. It was evident that complexes derived from L2H3 were inactive at 130 °C even after 24 h (Table 2, entries 1–4). When the temperature was increased to 160 °C, the activities substantially increased in all cases (Table 2, entries 9–12). For example, a 92% conversion was achieved using 4·2.25MeCN affording a polymer with Mn = 9000 with good control (PDI = 1.0) after 24 h (Table 2, entry 12). We also tested the catalytic behaviour of complexes 1–4 in the absence of BnOH at 130 °C and 160 °C. Interestingly, the results suggested that addition of BnOH has a negative effect on the polymerization rate and molecular weight (Table 2, entries 5–8 and 13–16). For a plot of conversion and time (min) for the polymerization of r-LA using 1–4, see Fig S14, ESI.† The kinetic study of the ROP of r-LA using 1–4 is shown in Fig. 7. The plot exhibited first order dependence on the r-LA concentration. The rate order observed is 4·2.25MeCN > 1 > 3·2MeCN > 2·0.5MeCN. The L2H3 derived Ta complex 4 showed the highest rate [Kobs = 17 × 10−4 min−1] followed by the L1H2 derived Nb complex 1 [Kobs = 11 × 10−4 min−1], L2H3 derived Nb complex 3·2MeCN [Kobs = 8.2 × 10−4 min−1] and the L1H2 derived Ta complex 2 [Kobs = 5.6 × 10−4 min−1]. Interestingly, for the ROP of r-LA, these results show that the Ta-based complex performs best when bound by the L2H3 derived ligand set, whereas the Nb system is superior in the case of the L1H2 derived ligand.
| Run | Cat. | [LA]0 : [cat.]0 : [BnOH]a |
T (°C) | Conv.b (%) | M n (calc.) | M n (obs.) | PDId | Pr |
|---|---|---|---|---|---|---|---|---|
| a [r-LA] = 10.00 mmol, [catalyst 1 or 2] = 0.01 mmol, [3 or 4] = 0.02 mmol, [BnOH] = 0.04 mmol (0.01 M in toluene), 24 h. b Determined by 1H NMR spectroscopy. c M n(calc.) = 144 × [LA]0/[Nb/Ta]0 × conv.% + Mendgroup, assuming one propagation chain per metal atom. d M n(obs) and PDI obtained by GPC in THF relative to polystyrene standards corrected by the Mark-Houwink correction factor Mnobs = MnGPC raw data × 0.58. e Pr is the probability of r dyad as determined by 2D homo J-resolved NMR spectroscopic analysis. | ||||||||
| 1 | 1 | 250 : 1 : 1 |
130 | 40 | 3708 | 1200 | 1.4 | — |
| 2 | 2 | 250 : 1 : 1 |
130 | 25 | 2358 | 900 | 1.6 | — |
| 3 | 3 | 250 : 1 : 1 |
130 | 3 | — | — | — | — |
| 4 | 4 | 250 : 1 : 1 |
130 | 11 | — | — | — | — |
| 5 | 1 | 250 : 1 : 0 |
130 | 72 | 6526 | 2700 | 1.3 | — |
| 6 | 2 | 250 : 1 : 0 |
130 | 39 | 3556 | 2000 | 1.2 | — |
| 7 | 3 | 250 : 1 : 0 |
130 | 4 | — | — | — | — |
| 8 | 4 | 250 : 1 : 0 |
130 | 46 | 8326 | 2300 | 1.3 | — |
| 9 | 1 | 250 : 1 : 1 |
160 | 77 | 7038 | 4500 | 1.1 | 0.50 |
| 10 | 2 | 250 : 1 : 1 |
160 | 55 | 5058 | 2000 | 1.2 | 0.46 |
| 11 | 3 | 250 : 1 : 1 |
160 | 65 | 11 808 |
9000 | 1.2 | 0.61 |
| 12 | 4 | 250 : 1 : 1 |
160 | 92 | 16 668 |
9000 | 1.0 | 0.36 |
| 13 | 1 | 250 : 1 : 0 |
160 | 93 | 8416 | 7200 | 1.3 | 0.51 |
| 14 | 2 | 250 : 1 : 0 |
160 | 87 | 7876 | 4000 | 1.9 | 0.50 |
| 15 | 3 | 250 : 1 : 0 |
160 | 89 | 16 066 |
8000 | 1.2 | 0.59 |
| 16 | 4 | 250 : 1 : 0 |
160 | 99 | 17 866 |
10 000 |
1.4 | 0.35 |
To determine the stereo-chemical microstructure of the PLA polymers, 2D homo J-resolved was employed and peaks were assigned by reference to the literature.28,29 For example, complex 4 gives isotactic PLA (Table 2, run 12 and 16, Pr = 0.35–0.36), while 3 shows a selectivity for heterotactic PLA (Fig. S15–S22, ESI†).
Polymer end groups were analysed by 1H NMR spectroscopy and MALDI-TOF mass spectra. For example, for the ROP of r-LA using 2·0.5 in the absence of BnOH in a 250
:
1
:
0 ratio, a series of peaks were observed with the main peaks identified as CH3CH2O– and OH end groups. The set of peaks, namely 144.13 n + 45 + 1.01 + 22.99, is attributed to (LA)n + –OCH2CH3 + H + Na+ (Fig. 8). From the 1H NMR spectrum, a quartet peak (e) at δ 4.15–4.20 ppm and a triple peak (f) at 1.27 ppm are consistent with the presence of the end group OCH2CH3, whilst the quartet peak (a) at δ 4.32–4.37 is the methine group of the other end group (Fig. 9).
![]() | ||
| Fig. 8 MALDI-TOF spectrum of the PLA obtained using 2·0.5MeCN (Table 2, entry 14). | ||
![]() | ||
| Fig. 9 1H NMR spectrum (400 MHz, CDCl3) of the PLA obtained using 2·0.5MeCN (Table 2, entry 14). | ||
:
[LA]
:
[cat] = [125]
:
[125]
:
[1] (i.e. CL
:
LA = 50
:
50). Results are summarized in Table 3.
| Run | First stage polymerization | Second stage polymerization | ||||||||
|---|---|---|---|---|---|---|---|---|---|---|
| First monomer | Time (h) | Conversion first monomer | Second monomer | Time (h) | Conv. CLa (%) | Conv. LAa (%) | M n(calc.) | M n(obs.) | PDIb | |
| [LA] = 3.46 mmol, [CL] = 3.46 mmol, [complex 4] = 0.028 mmol; solvent: toluene = 2 mL; temperature: 160 °C; reaction time: 48 h.a calculated from 1H NMR spectroscopy.b Mn(obs) obtained by GPC in THF relative to polystyrene standards corrected by the Mark–Houwink correction factor.c Mn(calc.) = MLA × [LA]0/[Ta] × %conv + MCL × [CL]0/[Ta] × %conv + Mendgroup. | ||||||||||
| 1 | CL | 12 | 52 | LA | 36 | 68 | 44 | 8851 | 6000 | 1.1 |
| 2 | CL | 24 | 88 | LA | 24 | 95 | 59 | 12 079 |
8000 | 1.3 |
| 3 | LA | 6 | 74 | CL | 42 | 99 | 99 | 16 000 |
11 000 |
1.5 |
| 4 | LA | 12 | 86 | CL | 36 | 37 | 95 | 11 232 |
8000 | 1.5 |
| 5 | LA | 24 | 94 | CL | 24 | 59 | 99 | 13 160 |
9000 | 1.2 |
| 6 | LA + CL | 48 | — | — | — | 94 | 95 | 15 294 |
13 000 |
1.4 |
To find an optimum reaction time for the copolymerization, the relationship between the conversion of the monomers and the reaction time following the addition of the first monomer was studied. It was found that when ε-CL was the first monomer added (12 h polymerization time), then following addition of r-LA and an additional 36 h, the conversions of ε-CL and r-LA were 68% and 44% respectively. On increasing the first monomer (ε-CL) reaction time to 24 h, the final conversion of ε-CL and r-LA reached 95% and 59%, respectively. It was evident that there was always an amount of unreacted r-LA when ε-CL was the first monomer added no matter how prolonged was the reaction time. It was evident here that the ROP of ε-CL was somewhat more difficult than that of r-LA. This is typified by the homopolymerization results whereby the activity of complex 4·2.25MeCN for ε-CL polymerization is rather low, and required 24 h to convert 250 equiv. of ε-CL to 88% monomer conversion at 160 °C, whilst 18 h was needed to convert 99% of the same amount of r-LA. The 13C NMR spectrum of the copolymer when ε-CL was the first monomer added and reacted for 24 h exhibits two carbonyl signals at 173.59 and 169.37 ppm, corresponding to the PCL and PDLLA block, respectively (Fig. 10(b)). The absence of any other peaks between these two carbonyl groups suggests no transesterification occurring in the polymerization.30
![]() | ||
| Fig. 10 Expanded 13C NMR spectra of copolymers prepared in sequential copolymerization of r-LA and ε-CL catalysed by 4·2.25MeCN. (a) Table 3, entry 3; (b) Table 3, entry 2; (c) Table 3, entry 6. | ||
In contrast, when r-LA was added first and then after 6 h ε-CL was introduced, 4·2.25MeCN was found to be an efficient initiator and could produce a block copolymer after 48 h with conversions for ε-CL and r-LA of 99% and 99%, respectively (Table 3, entry 3). Increasing the r-LA polymerization time to 12 h and 24 h reduced the conversion of ε-CL and led to transesterification. In the 1H NMR of PLA-b-CL (Fig. S23, ESI†), the expected signals for the copolymer were observed; the end groups of CH3CH2O– and OH were present. The 13C NMR spectrum of the copolymer exhibits two carbonyl signals at 173.63 and 169.45 ppm, corresponding to the PCL and PDLLA block, respectively (Fig. 10(a)).
For entry 6, we attempted the one-pot copolymerization of r-LA and ε-CL. After 48 h, the two monomers achieved high conversions of 94% for ε-CL and 95% for r-LA. The percentage of CL–LA heterodiads could be calculated from the 1H NMR spectrum by comparing the relative intensity of the methylene protons for CL–LA and CL–CL (Fig. S24, ESI†), and the percentage of CL–LA heterodiads was 94% suggesting the copolymers had random sequences.31 The chain microstructure of the copolymer was studied by 13C NMR spectrum (Fig. 10(c)); the carbonyl sequences were assigned according to the literature.30–34 The average lengths of lactidyl unit LLA and caproyl unit LCL can be calculated according to the equations as described by Kasperczyk.35 For PCL-co-PDLLA (Table 3, entry 6), LLA = 2.5 and LCL = 1.9, while LLA is slightly longer. The signal at 171 ppm, relating to the C–L–C sequence was not detected indicating the absence of second mode of transesterification.35 The molecular weights of the copolymers were lower than their theoretical values, with polydispersity in the range 1.1–1.5.
The two new families of niobium and tantalum complexes reported herein, add to the sparse number of examples reported to-date that utilize these metals in catalysts for the ring opening polymerization of cyclic esters.
Footnotes |
| † Electronic supplementary information (ESI) available: Alternative views of 1–4; IR and mass spectra; conversion v time plot; 1H NMR spectra of the polymers including 2D J resolved spectra of the PLA. CCDC 2150211–2150214. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d2nj02527b |
| ‡ Crystallographic data for 1–4. Crystal data for compound 1: C72H80Nb4O22, M = 1669, Monoclinic, space group C2/c, a = 22.2498(4), b = 14.4513(2), c = 25.8064(5) Å, V = 7575.3(3) Å3, Z = 4, Dc = 1.463 g cm−3, F(000) = 3408, T = 100(2) K, μ = 0.661 mm−1, λ(Mo-Kα) = 0.71075 Å, θmax = 57.396°, R1 ([I > 2σ(I)] = 0.0317, wR2 (all data) = 0.0856. For 2·0.5MeCN: C73H81.5N0.5Ta4O22, M = 2041.68, Monoclinic, space group C2/c, a = 22.2617(4), b = 14.3187(2), c = 25.8451(8) Å, V = 7491.0(3) Å3, Z = 4, Dc = 1.810 g cm−3, F(000) = 3964, T = 100(2) K, μ = 5.896 mm−1, λ(Mo-Kα) = 0.71075 Å, θmax = 57.400°, R1 ([I > 2σ(I)] = 0.0194, wR2 (all data) = 0.0475. For 3·2MeCN: C68H74N6Nb2O13, M = 1369.15, Monoclinic, space group C2/c, a = 54.0723(4), b = 10.74623(10), c = 22.47203(18) Å, V = 13041.45(19) Å3, Z = 8, Dc = 1.395 g cm−3, F(000) = 5680, T = 100(2) K, μ = 0.413 mm−1, λ(Mo-Kα) = 0.71075 Å, θmax = 57.400°, R1 ([I > 2σ(I)] = 0.0340, wR2 (all data) = 0.0881. For 4·2.25MeCN: C68.5H74.75N6.25Ta2O13, M = 1555.49, Monoclinic, space group C2/c, a = 54.1856(8), b = 10.7080(2), c = 22.4972(4) Å, V = 13038.2(4) Å3, Z = 8, Dc = 1.585 g cm−3, F(000) = 6236, T = 100(2) K, μ = 3.416 mm−1, λ(Mo-Kα) = 0.71075 Å, θmax = 58.702°, R1 ([I > 2σ(I)] = 0.0561, wR2 (all data) = 0.1510. |
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