Pierre-Luc Duranda,
Guillaume Cholletb,
Etienne Graua and
Henri Cramail*a
aLaboratoire de Chimie des Polymères Organiques, UMR 5629, CNRS, Universitè de Bordeaux, Bordeaux INP/ENSCBP, 16 Avenue Pey Berland, 33600, Pessac, France. E-mail: cramail@enscbp.fr
bITERG, F-33600, Pessac, France
First published on 21st December 2018
Bio-sourced polycarbonate networks have been synthesized from an alkene-functional fatty-acid based polycarbonate precursor. Cross-linked networks were created using the radical thiol–ene coupling reaction. The resulting polycarbonate materials exhibited versatile properties either influenced by the structure of the cross-linker or the cross-linker/olefin unit ratio. Indeed, the storage modulus above the glass transition temperature could be modulated from 0.9 to 8.9 MPa only by changing the type of cross-linker, i.e. 1,9-nonanedithiol vs. 1,4-benzenedimethanethiol. The cross-linker/olefin unit ratio was also shown to largely impact the polycarbonate networks properties. An elongation at break of nearly 200% was reached when a low cross-linker/olefin ratio was applied. Moreover, functional polycarbonate networks bearing pendant thiol groups were obtained when an excess of dithiol was used with respect to olefin groups.
Among the available bio-resources, vegetable oils appear as a very versatile platform for the design of polymer building blocks.2,3 Castor oil is one of the main renewable feed-stocks allowing the synthesis of bio-based polymeric materials, including, polyesters, polyamides, polyurethanes and many others.4
Recently, methyl 10-undecenoate, a commercially available castor oil derivative, was shown to be a suitable starting building-block to design original functional aliphatic polycarbonate (Fig. 1).5
In order to enhance the thermo-mechanical properties of these aliphatic polycarbonates, the present work is dedicated to the synthesis of versatile networks from these linear polycarbonate precursors.
Such polycarbonate networks exhibiting elastomeric properties are desirable thanks to a large number of applications in the biomedical area, especially in the emerging fields of soft-tissue engineering or drug delivery.6–11
Due to the presence of one dangling unsaturation per monomer units, thiol–ene coupling reaction appears to be a suitable method for the preparation of cross-linked networks.
Indeed, radical thiol–ene addition has been extensively employed for the cross-linking of functional polymers. For instance, Stevens et al. have exploited the thiol–ene reaction for the formation of nanosponges, through the cross-linking of copolymers.12 Truong et al.13 and Stevens et al.14 developed hydrogels with tunable properties including water uptake content, mechanical strength and degradation time by cross-linking poly(5-methyl-5-allyloxycarbonyl-trimethylenecarbonate) (PMAC) with a range of PEG-thiols. Finally, Barker et al.15 have used photo-initiated radical thiol–ene chemistry to produce 3D-printed structures based on polycarbonates via microstereolithography, as an alternative to potentially toxic acrylate-based printing systems.
The aim of this work is thus to investigate the influence of several parameters on the fatty acid-based polycarbonate network properties. First, different cross-linkers were used and investigations were performed to study their influence on the network properties. The influence of the cross-linker/olefin unit ratio on the network properties was also analyzed.
The Raman measurements were performed using a Jobin-Yvon Horiba XploRA confocal spectrometer with a resolution of 4.3 cm−1 in the spectral range 900–3100 cm−1. The laser source is a laser diode giving access to two laser wavelengths with a maximum power of 45 mW. Our work was carried out using an incident wavelength of λ = 785 nm and the laser beam power was fixed at 100% of the maximum power. To improve the signal-to-noise ratio, each spectrum was the result of 2 accumulated spectra with an acquisition time of 30 seconds for each spectrum.
To determine equilibrium swelling ratios and gel contents, strip-shaped specimens (0.6 mm thick, 0.5 mm width, 3 mm length) were placed in 10 mL of DCM for 24 hours. We assume that this procedure ensured complete removal of the sol fraction. Then the swollen gels were dried to constant weight at room temperature in vacuum and weighted.
The gel fraction (Fg) was calculated according to eqn (1) where md is the mass of dried (extracted) samples and m0 is the mass of the specimens before swelling.
(1) |
Dynamic mechanical analyses (DMA) were performed on RSA 3 (TA instrument). The sample temperature was modulated from −50 °C to 80 °C, depending on the sample at a heating rate of 4 °C min−1. The measurements were performed in a tension mode at a frequency of 1 Hz, an initial static force of 0.1 N and a strain sweep of 0.04%.
Tensile tests were performed on a MTS Qtest 25 Elite controller (France) at 20 °C. The initial grip separation was set at 20 mm and the crosshead speed at 50 mm min−1. The results were obtained from at least 3 replicates for each sample.
Fig. 3 Bio-based polycarbonate network (Table 1, entry 1). |
The aim of this study was to investigate both the influence of the type of cross-linker used and the cross-linker/olefin ratio on the polycarbonate network properties.
First, different cross-linkers were compared for a constant ratio dithiol/olefin ratio of 0.5 in order to get the highest cross-linking density (Fig. 2). P(NH-Und-6CC) was selected as starting polycarbonate, Irgacure 2959 as photoinitiator and 1,6-hexanedithiol (HDT), 1,9-nonanedithiol (NDT) and 1,4-benzenedimethanethiol (BDT) were used as cross-linkers. The use of 1,9-nonanedithiol should induce more space between the reactive groups and 1,4-benzenedimethanethiol should bring some rigidity between cross-linking points.
The mechanical properties have been evaluated by DMA and tensile tests. Results are summarized in Table 1.
Cross-linker | Gel content (%) | Tga (°C) | E′b (MPa) | Young modulusc (MPa) | Elongation at breakc (%) | Max stressc (MPa) |
---|---|---|---|---|---|---|
a Determined by DSC at 10 °C min−1 from the second cycle.b Evaluated with DMA analysis.c Calculated from tensile tests. | ||||||
HDT | 89 | 15.1 | 4.5 | 50 ± 4 | 76 ± 5 | 6.1 ± 0.8 |
NDT | 98 | 37.7 | 8.9 | 240 ± 20 | 25 ± 6 | 29 ± 3 |
BDT | 99 | 8.8 | 0.9 | 1.3 ± 0.1 | 190 ± 5 | 1.3 ± 0.1 |
All the materials display high gel content (≥89%) and rather low smell of dithiol testifying an almost complete cross-linking reaction. However, surprisingly, the network obtained with 1,9-nonanedithiol (NDT) exhibits a higher Tg (37.7 °C) and better mechanical properties (Young modulus of 240 MPa) than the network formed with 1,6-hexanedithiol (HDT) (Tg = 15.1 °C and Young modulus of 50 MPa) as seen from DMA curves (Fig. 4a) and stress–strain traces (Fig. 4b). Indeed, above the glass transition temperature, the storage modulus was much higher with NDT than HDT (increased from 4.5 to 8.9 MPa). On the contrary, when the rigid 1,4-benzenedimethanethiol (BDT) was used instead of HDT, a decrease of the network Tg (from 15.1 to 8.8 °C) and mechanical properties (storage modulus decreases from 4.5 to 0.9 MPa) was observed. The rigidity of the aromatic ring and the relative proximity of the reactive groups in 1,4-benzenedimethanethiol may hinder the access of the thiols to pendent olefins. In such a case, intramolecular coupling could occur resulting in a less cross-linked network. In contrast, the nine-carbon distance between the two thiol groups in 1,9-nonanedithiol makes carbon–carbon double bond more accessible. The so-formed network is thus fully cross-linked and displays higher mechanical properties, as confirmed by DMA tests. Indeed, the rubbery modulus plateau, which is proportional to the crosslinking density, is smaller for HDT than for NDT.
Fig. 4 (a) DMA curves and (b) stress–strain traces of polycarbonate networks obtained with different cross-linkers. |
These first experiments show that thermo-mechanical properties of the polycarbonate materials can be adjusted with respect to the type of cross-linker used (Fig. 5).
In the following, 1,6-hexanedithiol (HDT) was selected as a cross-linker to investigate the effect of the cross-linker concentration on the network feature. In theory, 0.5 equivalent of dithiol compared to the unsaturation should be added to entirely consume the total amount of unsaturations. However, in order to tune the 3D-polycarbonate properties, different cross-linker ratios have been investigated (Table 2).
Dithiol/olefin ratio | Tga (°C) | E′b (MPa) | Young modulusc (MPa) | Elongation at breakc (%) | Max stressc (MPa) | Gel content (%) | Swelling ratio (%) |
---|---|---|---|---|---|---|---|
a Determined by DSC at 10 °C min−1 from the second cycle.b Evaluated with DMA analysis.c Calculated from tensile tests. | |||||||
0.8 | 7.4 | 1.0 | 1.4 ± 0.5 | 121 ± 10 | 1.2 ± 0.5 | 83 | 214 |
0.5 | 15.1 | 4.5 | 50 ± 4 | 76 ± 5 | 6.1 ± 0.8 | 89 | 97 |
0.3 | 14.7 | 4.2 | 31 ± 5 | 64 ± 1 | 5.8 ± 0.5 | 86 | 102 |
0.2 | 8.6 | 2.0 | 2.4 ± 0.2 | 134 ± 12 | 2.2 ± 0.2 | 71 | 180 |
0.1 | 5.3 | 0.1 | 0.8 ± 0.2 | 175 ± 20 | 0.8 ± 0.1 | 34 | 283 |
The effect of the cross-linker concentration on gel contents and swelling ratios can be clearly seen. As expected, the gel contents and swelling ratios of the polycarbonate networks vary strongly with the cross-linker content. Indeed, the gel fraction of the network increases from 34% to 89% with an increase of HDT from 0.1 equiv. to 0.5 eq. Simultaneously, the swelling ratio in dichloromethane of the polycarbonate network decreased from 283% to 97%. It is important to note that an excess of cross-linker (0.8 equiv.) greatly increases the swelling ratio without decreasing the gel content meaning that the cross-linking density is lower.
As expected, the Tg increases when the dithiol/olefin ratio goes from 0.1 to 0.5. However, an increase to 0.8 equivalent of dithiol leads to lower Tg and lower storage modulus at the rubbery plateau, confirming that an excess of dithiol tends to decrease the cross-linking density of the network. It is speculated that pendent thiol groups which could not react with the unsaturations are probably present within the network (Fig. 6). This hypothesis is reinforced by the strong smell of the polycarbonate material even after several washes.
Fig. 6 Structure of the polycarbonate network when 0.8 equiv. of dithiol is added with 1 equiv. of olefin. |
In order to confirm the presence of pendent thiol groups, Raman spectroscopy was performed. The Raman spectrum (Fig. 7) exhibits the characteristic peak of thiol groups (around 2600 cm−1) even after several washings with phosphate-buffered saline (PBS), confirming the presence of such dangling functions grafted to the polycarbonate network.
The thermo-mechanical behaviour of the networks was determined by DMA, under tension mode. The storage modulus as a function of temperature for each polycarbonate network is shown in Fig. 9. These traces are indicative of amorphous cross-linked networks. At low temperatures, a glassy modulus plateau at 1 GPa is obtained. The glass transition region is recognized by the drastic decrease in modulus with increasing temperature. Beyond the glass transition region, the rubbery modulus plateau is nearly constant and, in accordance with the rubber elasticity theory, it is proportional to the cross-linking density of the network. We can clearly note, that the storage modulus at 50 °C decreases significantly from 4.5 MPa to 0.1 MPa by decreasing the number of equivalents of the cross-linker (from 0.5 to 0.1).
The difference between elastic modulus values is due to the different cross-link densities (ν) of networks defined as the number of moles of elastically effective network chains per cubic centimeter of sample, which can be calculated with the following eqn (2) with R = 8314 J mol−1 K−1, Tα+30 = 328.15 K and ϕ = 1.
(2) |
Fig. 8 exhibits the effect of cross-linker ratio (from 0.1 to 0.5) on the intensity of tanδ. Interestingly, the value of the alpha transition (Tα) is almost independent of the cross-linking density (around 25 °C). However, the intensity of tan delta peak varied significantly from 0.44 to 1.41 for 0.5 and 0.1 equivalent of dithiol, respectively. As the intensity reflects the extent of mobility of polymer chain at this temperature, the fact that tanδ intensity increases when the cross-linking decreases is coherent.
In addition, an excess of dithiol (0.8 equiv.) results in lowering the storage modulus at the rubbery plateau. This result confirms that an excess of cross-linker decreases the cross-linking density.
Nevertheless, the elasticity properties of the material can be modulated by tuning the cross-linker content.
The tensile properties of the polycarbonate network films are also given in Table 2 while representative stress–strain curves are shown in Fig. 10.
Fig. 10 Representative stress–strain curves of polycarbonate networks with different HDT/olefin ratios. |
It can be seen from these data that cross-linked polycarbonates exhibit different stress and strain at break values depending on the cross-linking density. Polycarbonate films containing 0.5 equivalent of cross-linker have stress at break values 7 times higher than the ones prepared with 0.1 equivalent of cross-linker (5.7 MPa and 0.8 MPa respectively). Strain at break values can be also modulated depending of the cross-linker content. The range of values goes from around 70% (with 0.5 equiv. of dithiol) to almost 200% (with 0.1 equiv. of dithiol). As expected, the excess of cross-linker decreases the mechanical properties of the so-formed polycarbonate network.
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