Synthesis and structural characterization
To study the hydrogen bonds, the samples were examined by FT-IR, and the results were shown in Figs. 2a-f. The peaks of 1684 and 1641 cm− 1 were attributed to the stretching vibration of disordered hydrogen-bonded -C = O and ordered hydrogen bonded -C = O respectively, while the peaks at 1570 cm− 1 were assigned to the hydrogen bonded in-plane bending vibration. In the other region, 3342 cm− 1 was the characteristic peak of -OH. In the FT-IR spectra of VanEHBP from 20 to 150 oC (Fig. 2a-b), the disordered hydrogen-bonded -C = O (1684 cm− 1) and ordered hydrogen bonded-C = O (1641 cm− 1) gradually decreased while the H-bond intensities of the free -C = O group at 1717 cm− 1 gradually increased. At the same time, the -OH characteristic peak shifted to higher wavenumber. Two-dimensional (2D) correlation analysis of FTIR spectra from 20 to 200°C were further performed, and the synchronous and asynchronous maps were shown in Figs. 2c-f. Four correlation cross peaks, that is, Φ(1728, 3364), Φ(1728, 3306), Φ(1652, 3364), and Φ(1652, 3306) were apparent in the synchronous spectrum and disappeared in the asynchronous spectrum, proving the existence of H-bonds in the dynamic networks32.
From the chemical structure of VanEHBP and CBA-TTE, the C = O groups of CBA-TTE and -OH of VanEHBP can form intermolecular hydrogen bonding (Fig. 3a). In order to further reveal thesupramolecular network structure of epoxy thermosets, molecular dynamics (MD) simulations were conducted to elucidate the cross-linking structures of EN-VanEP and EN-VanEHBP (Fig. 3b and c). The average cohesive energy per polymer chain for EN-VanEP and EN-VanEHBP are calculated to be 956.9 kJ·mol− 1 and 914.2 kJ·mol− 1 respectively. More specifically, the simulated revealed the number of H-bonds in EN-VanEHBP (151 per 2480 CBA-TTE units) are much higher than that of EN-VanEP (74 per 2480 CBA-TTE units), indicating the intermolecular interactions in EN-VanEHBP are much stronger than that of EN-VanEP. The hyperbranched topological structure of VanEHBP was favorable to the formation of H-bonds to induce higher-efficiency H-bonding interactions and denser H-bonds, as compared to the VanEHBP. Taken together, the hydrogen-bonding in supramolecular networks endows EN-VanEHBP with excellent mechanical properties, creep and chemical resistance.
Mechanical and thermal properties
Figure 4a displayed the tensile curves of epoxy thermosets, with the relevant data presented in Table S4. Obviously, EN-VanEP exhibited comparable mechanical properties as EN-DGEBA due to the similar structure of VanEP and DGEBA. The incorporation of VanEHBP simultaneously improved the mechanical properties and Tg of epoxy thermosets. With increase of the content of VanEHBP, the mechanical performance of epoxy thermosets first increased, reached maximum at 7 wt% VanEHBP, and then decrease. The tensile strength and toughness of EN-VanEHBP were 103.9 MPa and 3.58 MJ·m− 3, increased 43.1% and 132.5% respectively over the cured EN-VanEP (72.6 MPa and 1.54 MJ·m− 3). The effect of VanEHBP on the free volume (fv) of epoxy thermosets were studied by positron annihilation lifetime spectroscopy (PALS) and the results were presented in Table S5. Theincrease of fv in epoxy network was achieved through the incorporation of VanEHBP with large numbers of intramolecular cavities. In addition, epoxy chain segments crosslinked with VanEHBP extended in all directions, forming intermolecular cavities, which also helped to increase the fv. But the intermolecular hydrogen bonds restricted the chain mobility andtended to reduce the fv30,33,34, thus the fv of epoxy thermosets first decreased and then increased with increasing content of VanEHBP. The DMA curves of epoxy thermosets were shown in Figs. 4b and c, the storage modulus (Ec), Tg and crosslinking density (ρ) were listed in Table S4. The DGEBA has higher reactivity with curing agent than VanEP, thus EN-DGEBA exhibited higher Tg. The introduction of trimethylolpropane tris[poly(propylene glycol), amine terminated] ether as flexible aliphatic segment in VanEP decreased the rigidity of epoxy thermosets, thereby reduced the Tg. With the addition of VanEHBP, the Ec and crosslinking density increased first and then decreased. When 7 wt% VanEHBP was added, the Ec reached 2.8 GPa, and when the amount of VanEHBP was increased to 10 wt%, the Ec decreased to 2.1 GPa. The intermolecular hydrogen bonding with VanEHBP and FAT increased the crosslinking density of epoxy thermosets. However, the presence of non-crosslinkable cavities and flexible chain segment decreased the crosslinking density34,35. Thus, the Tg of EN-VanEHBP firstly increased and then decreased with gradually increasing content of VanEHBP. The SEM images of fracture surfaces of EN-DGEBA, EN-VanEP and EN-VanEHBP7 were presented in Figs. 4d-f. The smooth surfaces in the micrographs indicated brittle fracture of EN-DGEBA and EN-VanEP, while the rough, irregular surfaces of EN-VanEHBP7 suggest significant plastic deformation in ductile fracture. Figures 4g showed the AFM micrographs of EN-VanEHBP7 fracture surface, including height image, phase image, and three-dimensional image at a size of 5 µm × 5 µm. Only one phase was observed in the AFM topographical image (Fig. 4g). The mapping of phase image and three-dimensional image showed no phase separation.
The increased mechanical performance of EN-VanEHBP can be explained through supramolecular networks: (i) The hydrogen bonding interactions effectively stiffened and strengthened the materials. The reversible hydrogen bonds dissipated energy and redistributed stress before the failure, thus endowed EN-VanEHBP with high ductility and toughness. (ii) The deformation capability of intramolecular and intermolecular cavities provided efficient pathway to dissipate energy, leading to the stiff yet tough EN-VanEHBP. Meanwhile, the local free volume associated with hyperbranched crosslinks increased space for kink motions, and the crankshaft in strands made secondary relaxations possible. (ⅲ) The introduction of soft segments reduced the internal stress, and the arms of hyperbranched crosslinks could easily redistribute the forces reduce stress concentration. VanEHBP provided greater flexibility between crosslinks and increased the amount of conformational rearrangement during fracturing. Thereby, the as-developed supramolecular structural epoxy thermosets displayed outstanding mechanical performance.
Reprocessing and creep resistance
There were dual dynamic exchange reactions including imine exchange and transesterification in EN-VanEHBP (Fig. 5a). At elevated temperature, the exchange reactions of imine bonds and transesterification reaction promoted the topological rearrangement of EN-VanEHBP. Although the addition of VanEHBP increased the crosslinking density, which was unfavourable for the exchange reaction, the hydroxyl groups, high content of ester groups and the close-by statistical distance between dynamic exchange groups contributed to the mobility and rearrangement abilities of network segments. Thus, owing to the supramolecular networks, EN-VanEHBP could be easily reprocessed by compression moulding. Figures 5b-d depicted the time-dependent relaxation stress of EN-DGEBA, EN-VanEP and EN-VanEHBP (Fig. 5b) at different temperatures from 100 to 130 ℃. High temperature facilitated the movement of molecular segments, thus the relaxation rate increased as the temperature increased. The relaxation time of stress reached 1/e of the initial stress in stress relaxation curves treated with Maxwell model. As shown in the Fig. 5c, absolute stress relaxations were observed for EN-DGEBA, EN-VanEP and EN-VanEHBP7 at high temperature. For instance, the relaxation time of EN-VanEHBP7, EN-VanEP, EN-DGEBA reduced from 15 s, 47 s and 52 s to 10 s, 14 s and 18 s, respectively, when the temperature was raised from 100 to 130 ℃.
The values of activation energy (Ea) of exchange reaction were calculated using the following Eq. 36:
$$\text{ln}\tau =\text{ln}{\tau }_{0}+{E}_{a}/RT$$
1
where \({\tau }_{0}\) is the relaxation time, R is the gas constant (8.314 J·mol− 1K− 1). As shown in Fig. 5c, the curve of ln\(t\) vs. 1000/T was fitted to Arrhenius law. The Ea of EN-DGEBA, EN-VanEP, and EN-VanEHBP7 were calculated to be 44.8 K·Jmol− 1, 40.6 KJ·mol− 1 and 17.3 KJ·mol− 1, respectively. The value of Ea exhibited the same trend as the relaxation rate. As expected, the high content of dynamic bonds of EN-VanEP were conducive to the rearrangement of the molecular segments, and resulted in lower Ea and relaxation time than that of EN-DGEBA. The Ea of EN-VanEHBP further decreased with the addition of VanEHBP. The topology freezing transition temperatures (Tv) of epoxy thermosets were measured by DMA and the results were shown in Fig. 5d. If the samples were heated above Tv, the viscosity significantly decreased and exhibited Arrhenius-like viscosity variations like thermoplastic materials. So when the temperature exceeded Tv, samples featured weldability and malleability by rearranging the network topology37. The Tv of EN-VanEP was lower than that of EN-DGEBA, due to the rearrangement of EN-VanEP combined of imine exchange and transesterification. With the addition of VanEHBP, the exchange reactions were further promoted and the Tv of EN-VanEHBP gradually decreased with increasing content of VanEHBP. The exchange reaction was accelerated due to the following factors: (1) catalytic effect of hydroxyl groups from VanEHBP on transesterification, (2) higher concentration of ester groups of VanEHBPwhich was favourable for transesterification, (3) reduction of the statistical distance between reactive groups, (4) dissociation ofthe intermolecular hydrogen bonding at high temperatures which released chain mobility.As seen, EN-VanEHBP exhibited high dynamic exchange rate, excellent reprocessability and high Tg11,38–62. As a result of the fast exchange reactions, the fragments of EN-VanEHBP7 could be reprocessed into an integral film through hot press at 120 ℃ for 30 s under a pressure of 5 MPa (Fig. 5a). The mechanical and dynamic mechanical properties of the reprocessed samples were shown in Figs. 5e-f, Figure S10 and Tables S6-S9. The recover efficiency in terms of tensile strength was almost 100%. Similarly, the storage modulus and Tg were closed to those of the original samples after multiple reprocessing cycles, indicating that EN-VanEHBP7 could be well reprocessed and retain their original properties (Figs. 5e-f, Figure S10 and Table S6-9).
In order to study the dynamic imine exchange reactions, small model compounds were utilized. Firstly, model compounds A1A2 and B1B2 were synthesised with vanillin, m-toluidine, p-hydroxybenzaldehyde and aniline. Then the dynamic exchange between A1A2 and B1B2 were evaluated using GC-MS (Fig. 6). New species of A1B2 and B1A2 were obtained (within 30 min) through the associative and dissociative imine metathesis reactions between A1A2 and B1B2, which confirmed that the network rearrangement of imine exchange could readily proceed at relatively low temperatures.
Creep resistance was a key factor for EN-VanEHBP as engineering plastic and structure material. Creep performances of epoxy thermosets were tested under constant stress at different temperatures (Figs. 7a-c). After removing the stress, the deformation of EN-VanEP and EN-DGEBA could fully recover at temperature below 60 ℃. There was practically no creeping for EN-VanEHBP7 until the temperature was increased to 80 ℃ (Fig. 7d). Therefore, EN-VanEHBP showed better dimensional stability than EN-VanEP and EN-DGEBA. The cured EN-DGEBA, EN-VanEP and EN-VanEHBP7 samples were immersed into different solvents for 72 h at room temperature to further examine their solvent resistance (Figure S12 and Table S10). All the samples remained unchanged after being immersed in C5H12, CCl4, PhMe, H2O solution at 25 ℃ for 72 h. The better deformation resistance and chemical resistance of EN-VanEHBP is owing to the hydrogen bonds induced by VanEHBP.Thecross-linking from polymer chains by hydrogen bonds allowed EN-VanEHBP to be relatively immobile to withhold external forces in various environments, thus leading to improved creep and chemical resistance. Nevertheless, the network arrangement ability and dynamic properties were not affected at elevated temperatures due to the reversible dissociation of hydrogen bonds at higher temperatures.
Closed-Loop Recycling
As a special reversible chemical bond, the dynamic imine bond-based CANs can be degraded into oligomers containing aldehyde and amine groups under mild acidic conditions (Fig. 8a). As seen from Table S10, the swelling of epoxy thermosets in DMF were more pronounced than in other solvents (H2O, EtOH and THF). Therefore, we chose DMF as solvent for HCl aqueous solution degradation. The EN-VanEHBP7 samples were immersed into DMF with 0.1 M HCl aqueous solution (HCl aqueous/DMF = 1/10, v/v) at room temperature. After 180 min, the samples were depolymerised to orange and transparent degradation solution, then regenerated oligmers were obtained after removing the solvent. In order to further study the degradation of EN-VanEHBP7, the degradation solution, original and chemically recycled EN-VanEHBP7 were measured by FT-IR and NMR. As shown in Fig. 8b, depolymerized EN-VanEHBP7 had obvious aldehyde peak at 192 ppm in the 13C NMR spectrum, and the aldehyde peak at 9.83 ppm was also found in 1H NMR spectrum (Figure S13). Moreover, the solid-state NMR spectra of original and chemically recycled EN-VanEHBP7 exhibited similar patterns, and the imine bond peaks at 150 ppm in solid-state 13C NMR spectra were observed (Figure S13, 14), indicating that the recycled samples were of similar chemical structure as the original samples. To further verify the imine depolymerization, 600 mg EN-VanEHBP7 was immersed in a solution containing 9 mL DMSO-D6 and 0.9 mL 0.1 M HCl/DMSO-D6 solution (HCl/DMSO-D6 = 1/50, v/v) at room temperature and the degradation process was monitored by real-time 1H NMR (Fig. 8e). As shown in Fig. 8e, the CH = N proton peak (δ = 8.43 ppm) gradually decreased and new peak of CH = O (δ = 9.83 ppm) increased, indicating the successful dissociation of EN-VanEHBP7 at room temperature. By Calculating the integral area of the CH = O peak in real-time 1H NMR, it could be seen that the content of aldehyde increased and reached equilibrium after 100 min (Figure S15). The FT-IR spectra (S16, S17) also showed that the CH = N at 1643 cm-1 in the original samples disappeared and CH = O at 1683 cm-1 appeared in the degradation solution. The original sample and chemically recycled sample exhibited similar structure, demonstrating successful room temperature closed-loop recycling of EN-VanEHBP7. The tensile curves, storage modulus and tan δ vs temperature curves of original and regenerated epoxy thermosets were shown in Figs. 8c-f and Figure S18. The tensile curves of chemically recycled EN-VanEHBP7 were very close to that of the original sample, with a strength recovery efficiency of 93.5%. The storage modulus and Tg of the chemically recycled EN-VanEHBP7 were also almost the same as the original samples, exhibiting excellent room temperature closed-loop recyclability. Figure 8f showed that EN-VanEHBP7 exhibited the highest tensile strength among samples which can be recycled at room temperature2,36,37,63–70.