Open Access Article
Daniele
Giannantonio
,
Arianna
Brandolese
and
Andrew P.
Dove
*
School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2TT, UK. E-mail: a.dove@bham.ac.uk
First published on 20th December 2024
The permanent chemical structure that makes thermosets strong and stretchable materials also hinders their reprocessability and leads to their accumulation in the environment. To favour material reprocessability and reuse, polymers have been endowed with dynamic covalent bonds. However, when the dynamic bond is the network-forming bond, a significant trade-off between the robustness of the material and the dynamic behaviour can be encountered. In this study, nucleophilic thiol–yne click polymerisation was used to synthesise different materials possessing tuneable amounts of reversible disulfide bonds, thus achieving diverse thermomechanical properties. Furthermore, by leveraging different catalyst systems, the cis/trans conformer ratio on the backbone could be modulated to provide an additional degree of control over the thermomechanical properties. Finally, the presence of dynamic bonds was used as a handle to enable promotion of degradation and material reprocessing.
Recently, the introduction of dynamic covalent bonds into thermosets established covalent adaptable networks (CANs) as a new class of materials.6 The dynamic bonds within the materials can break and reform on sufficiently short timescales to allow the polymer chains to undergo molecular rearrangement, thus allowing macroscopic flow in a thermoplastic-like fashion. Parameters such as the nature of the dynamic bonds of choice (i.e. associative or dissociative) and the strategy deployed to form the network (step-growth vs. chain-growth polymerisation) influence the final architecture and bond distribution.7,8 Among the different dynamic bonds available, disulfide bonds have received significant attention because of their widespread presence in biological systems and well characterized dynamic behaviour.9,10 With a dissociation energy of around 60 kcal mol−1, lower than that of the aliphatic C–C bond of 80–90 kcal mol−1, disulfide bonds provide a good balance between dynamicity and robustness.11,12
In light of their efficiency, several thiol-based reactions have been used for the synthesis or functionalisation of polymeric materials.13 Among these, the use of thiol–ene Michael addition, radical or nucleophilic, arguably represents the most common approach given its simplicity and functional group tolerance.14–16 Because of the reversibility of the thia-Michael adduct, several CANs built on this reaction have been reported.17–20 Similarly, the use of activated alkynes allows for the nucleophilic thiol addition across the triple bond.21–26 Only recently, Du Prez and co-workers reported the use of nucleophilic thiol–yne addition to activated alkynes to obtain CANs with tuneable relaxation rates depending on the electronic of the alkyne of choice.27 While this work shows that network formation can be achieved through the use of a reversible reaction, only dissociative bonds can be introduced with this approach thus limiting its scope. Moreover, since bifunctional alkynes and thiols are being used, the thiol–yne addition reaction is responsible for the formation of pre-polymers, and only a subsequent thiol–ene addition forms the crosslinked structure.
The use of such a selective reaction represents an advantage because of its efficiency, high yield, and tolerance towards a wide range of functional groups. Additionally, if the presence of the dynamic bonds is independent of the polymerisation method, a greater range of reversible moieties can be introduced.28 Moreover, when a bifunctional alkyne is reacted with a multifunctional thiol (functionalities >2), the prepolymer synthesis step can be bypassed simplifying the network formation. Previous work showed that the ratio of the resulting addition products, the trans and cis isomers, can be modulated by catalyst and/or solvent selection. In fact, cis-enriched products have been synthesised increasing solvent polarity or switching to stronger bases as catalysts.16,29 This is particularly interesting as backbone cis/trans isomerism has been previously used to tailor thermomechanical performances in linear polymers,30–32 hydrogels,33 and 3D printable resin,34 but this concept has not, to date, been applied to CANs. Herein, a bifunctional propiolate possessing an internal dynamic disulfide bond (C2SS) was here successfully introduced into crosslinked materials by reaction with a three-arm thiol (Fig. 1). The thermomechanical properties of the resulting network were found to change according to the ratio of the monomers and cis/trans content. Finally, the presence of dynamic disulfide bonds rendered these materials degradable and reprocessable.
![]() | ||
| Fig. 1 Scheme representing the network formation and the influence of the catalyst on cis/trans isomerism (top) and the monomers used in this work (bottom). | ||
:
1: C2SS
:
C6, and 100% C6 respectively) while keeping the stoichiometric ratio between alkyne and thiol groups 1
:
1. trans-Net(3-AT1.5-C2SS1) was accessed by reacting monomer C2SS with 3-AT in equimolar amounts, to have a thiol
:
alkyne ratio of 1.5
:
1. Lastly, cis-rich networks NetC2SS and NetC6 (100% C2SS and 100% C6 respectively) were accessed by employing DBU as the catalyst of the reaction.29,30 Consumption of the alkyne bonds following thiol–yne addition was confirmed by Fourier-transform infrared (FTIR) spectroscopy on the free-standing films, confirming the disappearance of the relative stretching bands (Fig. 2A and B). The formation of networks was further confirmed by performing swelling experiments at room temperature in CHCl3. All networks displayed high gel content (>80%) and a swelling ratio above 250% confirming nucleophilic thiol–yne polymerisation as an excellent tool for the synthesis of crosslinked materials (ESI, Table S1†).
δ) of the different networks. The broad and bimodal tan
δ curves displayed by the 1
:
1 thiol
:
alkyne ratio networks suggest that the networks possess a non-homogeneous structure, however, no drop in modulus was recorded (Fig. 3A) which suggests that all materials showed excellent dimensional stability in the temperature range tested (−80 °C to 130 °C). Notably, trans-NetC2SS did not display any loss in modulus even at temperatures as high as 180 °C (ESI, Fig. S6†). The absence of a significant drop in modulus above Tg, indicative of a gel-to-sol transition and typically found in dissociative CANs, suggests that these materials behave in an associative “vitrimer-like” fashion.35,36 The same behaviour has been observed in many CANs possessing both aliphatic37–39 and aromatic40–43 disulfide bonds. Nonetheless, a significant decrease in stress could be observed for trans-NetC2SS, when stress-relaxation experiments at higher strain (10 μm vs. 1 μm) were performed at 150 °C (Fig. 3B). Full relaxation, determined as the time corresponding to ∼37% of the initial stress value following a Maxwell model,44 was reached in roughly 18 minutes. This behaviour was attributed to the dissociation of the disulfide bonds, as trans-NetC6 modulus remained constant throughout the experiments. The relatively slow dissociation was linked to the aliphatic nature of the disulfide bonds, which display higher stability when compared to aromatic disulfides.11 Even so, this relaxation is consistent with other works displaying aliphatic disulfides. For example, Zhang and colleagues reported variable relaxation rates going from 1.5 s (200 °C) to 90 minutes (60 °C) in a system containing aliphatic disulfide and ester bonds.39 All materials displayed rubbery behaviour above their glass transition temperature (Tg), as the tan
δ dropped to 0.
When compared to trans-NetC2SS, trans-Net(3-AT1.5-C2SS1) displayed a monomodal and narrower tan
δ curve, suggesting that a 1.5
:
1 ratio between thiols and alkyne leads to a more homogeneous network. The decreased molecular weight between crosslinking (Mc) (Table 1) and lower swelling ratio (ESI, Fig. S7 and Table S1†) support this hypothesis, however, very few differences regarding Mc were found among the networks, suggesting that these systems are comparable. The limit of the viscoelastic region (LVE) and yield point determined via rheology were found to be similar, as shown by amplitude sweeps performed on the high-trans networks (ESI, Fig. S8†). Frequency sweeps confirmed the reduced influence of different degrees of crosslinks on shear stress as the networks did not display strong differences (ESI, Fig. S9†). It is important to note that the density of the material was assumed to be 1 g mL−1, and the theory of rubber elasticity showed some limitations with highly crosslinked systems.45,46 These data suggest that as different monomer C2SS and C6 ratios were explored, the composition may be responsible for the differences regarding mechanical behaviour, however, when more homogeneous network structures are achieved, these differences can be offset. In fact, trans-Net(3-AT1.5-C2SS1) was able to compete with a fully carbon–carbon based network such as trans-NetC6.
| Name |
T
g a [°C] |
b [MPa] |
M c [g mol−1] |
E c [MPa] |
σ at break (UTS) [MPa] | ε at break [%] | Strain energy densityd [J m−3] |
T
g e [°C] |
T
d, 5% f [°C] |
|---|---|---|---|---|---|---|---|---|---|
a Determined as the peak of the tan δ curve.
b Taken as the value associated with Tg + 50 °C.
c Determined as the slope of the curve at 1% strain.
d Determined as the area below the stress vs. strain curve.
e Determined as the inflexion point of the second heating cycle of the DSC thermograms.
f Determined as the temperature associated with a 5% mass loss.
|
|||||||||
| trans-NetC2SS | 7.25 | 239.7 | 34.5 | 0.73 ± 0.17 | 0.63 ± 0.06 | 94.8 ± 22.2 | 0.34 ± 0.12 | −7.4 | 186.2 |
| trans-NetC6 | 13.2 | 1314.2 | 6.39 | 0.77 ± 0.4 | 1.35 ± 0.39 | 72.5 ± 21.9 | 0.59 ± 0.28 | −7.4 | 337.8 |
| trans-Net(C2SS-C6) | 4.33 | 506.5 | 16.1 | 2.03 ± 0.11 | 2.56 ± 0.15 | 155.4 ± 12.6 | 2.2 ± 0.3 | −10.4 | 300.5 |
| trans-Net(3-AT1.5-C2SS1) | 4.8 | 1186.4 | 6.9 | 3.4 ± 0.7 | 1.3 ± 0.6 | 51.2 ± 25.4 | 0.39 ± 0.31 | −14.4 | 192.2 |
| cis-NetC2SS | 13.25 | 302.4 | 27.7 | 2.5 ± 0.4 | 3.7 ± 1.9 | 235.7 ± 101.7 | 4.9 ± 3.7 | −3.2 | 171.8 |
| cis-NetC6 | 10.5 | 720.3 | 11.6 | 0.93 ± 0.56 | 5.7 ± 2.5 | 471.7 ± 121.9 | 10.7 ± 5.3 | 1.3 | 316.3 |
cis-Rich networks showed different properties when compared to their trans-rich analogous. While cis-NetC2SS displayed a slightly higher rubbery storage modulus (
) than trans-NetC2SS, cis-NetC6 possessed a lower
value when compared to trans-NetC6. Taken together, these results suggest that different degrees of cis/trans isomerisation can alter the modulus of thermosets, but this effect is mediated by composition as well (Table 1).
Further probing of the mechanical properties was performed via uniaxial tensile testing on dogbones cut from the cast films (Fig. 3C, Fig. S10–S15† and Table 1). Despite its lower Mc, trans-NetC2SS was found to possess a similar Young's modulus (E) and elongation at break (ε) to trans-NetC6. trans-NetC6 displayed a slightly higher ultimate tensile strength (UTS) (ESI, Fig. S16–S18†), which is likely a result of its higher carbon–carbon bond content.11,12 To our surprise, trans-Net(C2SS-C6) displayed higher UTS and elongation at break than either network formed from a single alkyne monomer, (ESI, Fig. S16–S18†) demonstrating that subtle changes to the chemical composition can significantly alter mechanical performance of the resultant materials. When compared to trans-NetC2SS, trans-Net(3-AT1.5-C2SS1) displayed higher Young's modulus (E = 3.4 ± 0.7 MPa vs. E = 0.73 ± 0.17 MPa, Fig. S16†) and stress at break (σ = 1.3 ± 0.6 MPa vs. σ = 0.63 ± 0.06 MPa, Fig. S17†), but lower elongation (ε = 51.2 ± 25.4% vs. ε = 94.8 ± 22.2%, Fig. S18†). These results are consistent with the higher crosslinking density associated with trans-Net(3-AT1.5-C2SS1), which is also corroborated by its lower swelling ratio (ESI, Table S1†).
Both cis-rich networks showed enhanced UTS than their trans-rich counterparts, confirming that stereochemistry can alter the mechanical properties of thermosets. When compared to trans-NetC2SS, cis-NetC2SS also displayed significantly higher Young's modulus (ESI, Fig. S16†), while cis-NetC6 showed higher elongation at break with respect to trans-NetC6 (ESI, Fig. S18†). Comparing the two, cis-NetC2SS displayed a higher Young's modulus than cis-NetC6 (ESI, Fig. S16†), but no statistically significant differences were observed in stress and strain at break when comparing the results via an unpaired T test. However, it is noticeable from the stress–strain curves that the strain at break of cis-NetC6 is almost double that displayed by cis-NetC2SS, suggesting that further evaluation into the presence of architectural defect could lead to more pronounced differences, underlying once again the trade-off between dynamic behaviour and mechanical performances (ESI, Fig. S17 and S18†). These results suggest that increasing cis-content leads to materials possessing a higher strain energy density (Table 1). This may be explained by mechanically induced cis-to-trans isomerisation, which was probed by Radiom and co-workers.47 The authors described that when cis-rich norbornene polymers were stretched via atomic force microscopy (AFM), an increase in extension was measured because of the isomerisation of the shorter cis linkages into the longer trans conformation, which resulted in relaxation of the force. From a material point of view, this event could lead to energy dissipation, thus allowing the material to withstand greater stress. Notably, trans-Net(C2SS-C6), cis-NetC2SS, and cis-NetC6, displayed ultimate tensile strength and elongation comparable to the likes of styrene butadiene rubber (SBR) and ethylene propylene diene monomer (EPDM), two commonly used elastomers.48
Differential scanning calorimetry (DSC) revealed all the networks to be amorphous as no melting transition was detected (Fig. 4B and ESI, Fig. S20–S25†). While the higher degree of crosslinking is generally associated with an increase in glass transition temperature (Tg), trans-NetC6 underwent transition at the same temperature as trans-NetC2SS (−7.4 °C). However, when both monomers were used to synthesise trans-Net(C2SS-C6) its Tg was recorded 3 °C lower at −10.4 °C. Tg of trans-Net(3-AT1.5-C2SS1) was determined at −14.7 °C, roughly 7 °C lower than trans-NetC2SS. These observations can be rationalised as a result of unreacted thiols within the network acting as chain-ends, thus increasing the free volume of the network. Both high-cis networks revealed Tgs higher than their high-trans counterparts, confirming that cis/trans isomerism can also be used to modulate the thermal properties of the thermosets (Table 1).
Finally, reprocessing of these crosslinked materials was demonstrated by heat compression moulding. trans-NetC2SS fragments could be moulded into a free-standing film by heat compression moulding at 150 °C for 20 minutes at a pressure of 3000 kg. The same was possible for trans-NetC6, albeit the reprocessed films were less structurally stable. This supports the conclusion that the inclusion of disulfide bonds is the primary driving force of the dynamic behaviour of these materials (ESI, Fig. S31†). Neither network displayed the same homogeneity as the virgin analogues, which suggests that the network structure was not perfectly reformed, possibly in light of the thermal degradation of the catalysts or of the network itself.51
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4py01195c |
| This journal is © The Royal Society of Chemistry 2025 |