Synthesis and characterization
A bio-based α,ω-difunctional diene 1 was synthesized by combining structurally rigid isomannide and flexible undecenoic acid (Fig. 2a). 1 can undergo acyclic diene metathesis (ADMET) polymerization to produce a polyester. Despite considerable efforts on this reaction, the stepwise polymerization mechanism posed challenges in achieving the desired molecular weight as a result of limited conversion. This limitation resulted in the achievement of only a modest molecular weight, as evidenced in Supplementary Table S1. We selected the sample with the highest molecular weight (P1, Mn=23.3 kDa, Table 1) for testing. The presence of linear alkyl chains derived from undecenoic acid can lead to the formation of crystalline polymers. As expected, P1 shows the ability to crystallize with a low melting enthalpy (5.0 J/g, Supplementary Fig. S4), indicating a low crystallinity. The mechanical property test demonstrated a characteristic behavior of elastic materials (with a low Young’s modulus of 0.22±0.05 MPa) but exhibited poor mechanical strength (0.03±0.01 MPa, Supplementary Fig. S6) due to its low molecular weight that lack significant entanglement.22 This polymer could undergo ring-closing metathesis depolymerization to yield a cyclic olefin 2 (trans-isomer dominated, in accordance with their ring strain, Supplementary Fig. S7), the same product as obtained from the diene under ring-closing metathesis conditions (Supplementary Fig. S8). This cyclic olefin 2, as a product for upgrading the recycling of P1, could be used in ring-opening metathesis polymerization (ROMP) via the chain growth polymerization mechanism.23-27 Due to the low ring strain of this monomer (~4 kcal mol-1, Supplementary Table S4), the polymerization is favored by high monomer concentration, which progressed smoothly with quantitative conversion (>95%) under mild conditions (at 25 oC within 1 h under 1.0 M condition). The molecular weight can be adjusted with the reaction time or the monomer-to-catalyst feeding ratio (Supplementary Table S2), providing greater control and enabling the production of TPEs with high molecular weights (Table 1, P2−P9, 40 kDa−800 kDa) with enhanced chain entanglement. The improved molecular mass could allow finding outstanding and unique mechanical properties.
Table 1 Polymers prepared by metathesis polymerization
|
Mna (kDa)
|
Đa
|
Eb (MPa)
|
ΔHmc (J/g)
|
Td,5%d (oC)
|
σbb (MPa)
|
εbb (%)
|
P1
|
23.3
|
1.73
|
0.22±0.05
|
5.0
|
387.5
|
0.03±0.01
|
525±186
|
P2
|
46.0
|
1.88
|
0.20±0.03
|
7.7
|
375.2
|
1.40±0.2
|
581±50
|
P3
|
103.6
|
2.16
|
2.04±0.87
|
26.2
|
416.1
|
17.1±2.8
|
910±34
|
P4
|
158.3
|
2.10
|
1.86±0.18
|
24.5
|
415.2
|
31.5±3.1
|
1495±286
|
P5
|
227.8
|
2.28
|
2.09±0.70
|
21.2
|
426.5
|
22.7±1.7
|
1361±320
|
P6
|
303.0
|
2.40
|
1.98±0.61
|
20.7
|
414.7
|
21.7±0.7
|
1155±172
|
P7
|
648.1
|
2.97
|
2.65±0.11
|
19.8
|
403.5
|
19.8±1.1
|
924±112
|
P8
|
722.0
|
2.85
|
1.29±0.23
|
14.3
|
401.8
|
17.4±0.5
|
1378±328
|
P9
|
794.2
|
2.55
|
1.42±0.65
|
10.9
|
392.4
|
12.5±1.3
|
894±220
|
P10e
|
106.1
|
1.80
|
43.11±1.1
|
80.0
|
398.6
|
5.80±0.4
|
1438±100
|
P11f
|
310.5
|
2.53
|
3.56±0.98
|
36.6
|
407.3
|
12.9±1.3
|
673±75
|
rP4
|
141.9
|
2.08
|
2.04±0.64
|
22.2
|
402.8
|
28.7±1.5
|
1480±173
|
aDetermined by gel permeation chromatography (GPC) in THF, calibrated with polystyrene standards.
bDetermined by tensile test at a strain speed of 10 mm/min.
cDetermined by DSC during the heating scan.
dDetermined by TGA with decomposition temperature at 5% weight loss.
eIsomannide along the homopolymer backone was replaced by pentanediol.
fIsomannide along the homopolymer backone was replaced by isosorbide.
Thermal properties
To validate the role of isomannide in elastomer formation, a control polymer P10 was prepared by replacing isomannide with a pentanediol motif having a similar contour length but better segmental flexibility (Fig. 2b). A melting peak at 41 °C and a Tg at −21 °C are observed for P4, indicating noticeably reduced crystallinity compared to P10 (Fig. 2c), as evident from the low melting enthalpy (24.5 J/g) and the XRD diffraction pattern of P4 (Fig. 2d and Supplementary Fig. S10, χc=17%). Unlike high-density polyethylene (HDPE), where the diffraction peaks at 21.4o and 23.7o in Fig. 2d are primarily attributed to polyethylene (110 and 200 lattice planes),28 a prominent peak at 19.5o in P10 indicates the presence of pentanediol ester moieties within the crystalline lamellae. In contrast, P4, which contains bulky isomannide groups along the backbone, displays dominant diffraction peaks at lower angles, suggesting extensive participation of isomannide moieties in crystallite formation. In the chain ordering process of P4, the formation of the amorphous domain leads to defects that significantly impede the thickening of the crystalline lamellae, resulting in a decrease in crystallinity.29 When examined under a polarized optical microscope (POM, Fig. 2e), P4 demonstrates pronounced birefringence, indicating the presence of crystals. The crystal size in P4 falls within the micrometer range, providing it with notable transparency, as depicted in Fig. 2b. Furthermore, P4 exhibits excellent thermal stability, with a degradation temperature at 5% weight loss (Td,5%) that reaches 415 °C (Fig. 2g). The thermal stability of all elastomers is comparable to that of HDPE (Supplementary Fig. S23).
Mechanical Properties
To investigate the mechanical properties of these polymers, uniaxial tensile testing was performed. P2−P9, which feature isomannide along the backbone, exhibit elastomeric behavior with a low Young’s modulus (~2 MPa) as depicted in Fig. 3a. Replacement of isomannide with its stereoisomer isosorbide can also produce a TPE (P11, Table 1, Supplementary Fig. S24). However, P10, with pentanediol along the backbone, shows a significantly higher Young’s modulus (43.1 MPa) and undergoes plastic deformation through necking during stretching. This highlights the crucial role of the bulky group in the creation of tough elastomers within these materials. Remarkably, the mechanical strength and elongation at break of these elastomers peak at 32 MPa and 1500%, respectively, surpassing those of many known recyclable TPEs as shown in Fig. 3b.11, 13-19, 30 The thermomechanical properties of this material are similar to those of conventional TPEs such as SBS (styrene-butadiene-styrene) and SEBS (styrene-ethylene/1-butene-styrene) block copolymers,31 making them competitive alternatives with the added benefit of chemical recyclability. This exceptional performance for isomannide-based polymers is primarily attributed to their unique slightly crystalline structure. In this structure, an amorphous rubbery matrix with significant interchain entanglement envelopes the crystalline domains (Fig. 2f). The amorphous domains provide the initial softness and high extensibility of the material, whereas the crystallites act as strong physical cross-links, reinforcing the overall network. Furthermore, the highly entangled amorphous chains act as tie-chains connecting the small crystalline domains.32
Structure-property relationship
The mechanical strength of elastomers is influenced by several factors, including a high molecular weight and a high content of hard segments,33 which correspond to crystallinity in this work. P1–P9 exhibit a high trans carbon–carbon double bond content along the polymer backbone (Supplementary Tables S1 and S2). The slight difference in stereoselectivity (80%±7%) between them is not expected to have a significant impact on their inherent crystallinity. It is worth noting that, while higher molecular weights and an increase in hard blocks are generally associated with enhanced material strength, an increase in molecular weight may paradoxically lead to a reduction in polymer crystallinity.34 According to the data shown in Fig. 3c, for the P1−P9 polymers, a nonmonotonic stress at break trend is observed, showing a peak (σb of 32 MPa) at a molecular weight of 158 kDa. Following this peak, the tensile strength decreases as the molecular weights increase, a pattern that aligns closely with the corresponding crystallinity values shown in Fig. 3d. The mechanical strength of the elastomer is primarily influenced by the molecular weight within the range of 100 kDa to 158 kDa. Once the critical molecular weight threshold is exceeded, the significance in determining the mechanical strength shifts from entanglement density to crystallinity. Therefore, the interplay between the density of amorphous entanglements and the stability of crystal blocks ultimately determines the mechanical strength of the homopolymer-based elastomers.35
The elastic performance of the toughest elastomer, P4, was further assessed by cyclical tensile tests, where the sample was stretched to 100% strain and relaxed at a rate of 100 mm/min. For clarity, the curves of each cycle are shifted on the strain axis (Fig. 3e). The P4 sample sustained excellent elastic recovery (>98%) during ten-cycle tensile deformations (Supplementary Fig. S25). The resilience of P4 was also improved during the cyclic tensile deformation processing (Supplementary Fig. S26), leading to a perfection of the network structure.36 Step-cycle tensile tests were also performed on P4 (Fig. 3f). The continuous drop in modulus with strain indicates a typical strain-evolving structure of P4,37 in which the crystals undergo yielding to break into smaller domains.38 The isolated crystals generated make the stiffness of the material being dominated by the entanglement amorphous phase, thus leading to an elastomeric-like structure with good elastic recovery (~90%, Supplementary Fig. S27). Stretching of chain segments and strain-induced crystallization (Supplementary Figs. S29 and S30) are responsible for strain hardening after large deformation, resulting in ultrahigh mechanical strength.
Recycling studies
When performing temperature-dependent polymerization thermodynamic studies, the prepared elastomers exhibited a relatively high Tc (1731 oC at 0.15 M, details in Supplementary Figs. S1–S3). At a concentration of 0.15 M, the Gibbs free energy value (ΔG) for 2 polymerization was observed to be -3.14 kcal mol-1 at 25 °C, indicating a more favorable outcome compared to many reported depolymerizable polyolefins prepared through ROMP.39, 40 When diluted in a solvent, the Tc can be lowered to allow depolymerization under mild conditions.41 Consequently, high conversions were anticipated for both forward polymerization and reverse depolymerization processes. To demonstrate a closed chemical recycling loop, 10.0 g of P4 underwent polymer-to-monomer recycling under mild conditions (concentration of repeat units = 20 mM, 50 °C, 1 h) in the presence of 1 mol% Grubbs second generation catalyst (G2). The ring-closing metathesis depolymerization process proceeded smoothly with more than 99% conversion, resulting in a viscous liquid mixture of diverse ring-sized macrocycles. This outcome indicated an equilibrium between the various cycles,42, 43 as supported by GPC elution curves (Fig. 4b) and high-resolution mass spectrometry (HRMS) results (Fig. 4d). NMR and mass spectrometry analyzes confirmed that the major depolymerization products were monomers (56% yield, Supplementary Figs. S31-S33). The depolymerization kinetic analysis revealed complete degradation of the pristine polymer within 15 minutes, followed by further transformation of the oligomeric macrocycles into monomer species until equilibrium was reached at 1 hour (Fig. 4c). Component fractions were determined by integrating GPC refractive index (RI) traces, closely aligned with the 1H NMR integration (Supplementary Fig. S35). After removing the residual catalyst, the depolymerized mixture of macrocyclic oligomers could be directly repolymerized via ROMP to recover virgin polymer with high molecular weights (Supplementary Fig. S38 and Table S5). The conversion was found to be quantitative according to the 1H NMR and GPC analyzes (Supplementary Figs. S36 and S37). In particular, 9.2 g of recycled polymer (rP4, Table 1) were obtained, resulting in a quantitative polymer-to-polymer chemical recycling ratio of 92% (Fig. 4b). The structural integrity of rP4 closely resembled that of pristine P4 (Figs. 4a and 4b), leading to similar thermomechanical properties (Fig. 4e and Supplementary Fig. S23).
To further understand the depolymerization thermodynamics and optimize the depolymerization conditions (including temperature, catalyst type, catalyst loading ratio, and concentration), the monomer recovery ratio was utilized. An increase in monomer recovery efficiency with higher depolymerization temperatures aligns with the entropy-driven nature of depolymerization at this low concenration (concentration of repeat units = 20 mM, Supplementary Fig. S40). Among different Grubbs catalysts (G1, G2, G3, and HG2), G3 demonstrated a superior efficiency over G2, achieving the highest monomer recovery ratio of 62% (Supplementary Fig. S42). A catalyst loading ratio greater than 0.5 mol% was considered sufficient (Supplementary Fig. S44). The dilute concentrations significantly changed the equilibrium towards monomer formation, particularly at a concentration of 1 mM concentration, where the monomer yield exceeded 90% (Supplementary Fig. S46). In particular, the monomer recovery ratio did not exhibit dependence on molecular weight (Supplementary Fig. S48), suggesting the feasibility of scaling up depolymerization through a one-pot strategy for a mixture of elastomers with varying molecular weights (a mixture of P1−P9), which was previously unattainable when recovering multicomponent elastomers. The depolymerization of the elastomer specimen mixtures in the presence of G2 demonstrated successful recovery of monomers. Treatment of crude reaction products with DMSO, followed by filtration through a short silica plug, effectively eliminated colored ruthenium by-products and oligomer fractions, leading to recovery of high-purity monomers (HPLC>99%, Supplementary Figs. S49 and S50).
The ester group within the polymer chain can also serve as a breaking point, allowing degradation through hydrolysis in a conventional manner. Gentle heating of these elastomers in an alkaline aqueous solution for several hours leads to a quantitative recovery of isomannide and unsaturated telechelic diacid (93% yield, Supplementary Figs. S51−S53), which can then be used to produce industrially valuable α,ω-dicarboxylic acids. The resulting hydrolyzed products can undergo polycondensation to regenerate the virgin polymer (Supplementary Fig. S54), although with limited molecular weight.44 In summary, three synthesis loops are established based on the linkages that react from the original isomannide and undecenoic acid feedstock (Fig. 5): one involves hydrolysis, esterification, and ADMET polymerization (Cycle 1); another encompasses hydrolysis and polycondensation (Cycle 2); and the third involves cyclodepolymerization and ROMP (Cycle 3).