Alexandra L.
Mutch
* and
Stuart C.
Thickett
*
School of Natural Sciences – Chemistry, University of Tasmania, Hobart 7001, Tasmania, Australia. E-mail: Alexandra.mutch@utas.edu.au; stuart.thickett@utas.edu.au
First published on 12th February 2025
The preparation of interpenetrating polymer networks (IPNs) and semi-interpenetrating polymer networks (semi-IPNs) is reported via a solvent-free approach using a binary polymerizable eutectic. N-Isopropylacrylamide (NIPAM) and ε-caprolactone (CL) were mixed in various mole ratios to prepare viscous polymerizable liquids that were stable at room temperature, based on solid–liquid equilibrium phase diagrams from differential scanning calorimetry (DSC) data. The strong degree of association between NIPAM and CL within these mixtures was confirmed via 1D and 2D NMR spectroscopy. Using an appropriate UV photoinitiator and ring opening polymerization catalyst, the orthogonal polymerization (either in a sequential or simultaneous fashion) of each component within the eutectic was achieved, with enhanced reaction kinetics for the ring opening polymerization compared to a traditional solvent (DMSO). Through the incorporation of diacrylate and bis(carbonate) crosslinkers into the resin mixture, IPNs and semi-IPNs were realised in a one-pot two-step approach from polymerizable eutectics for the first time. These networks possessed thermoresponsive swelling behaviour in water, and retained their structural integrity in good solvents for both phases. This binary eutectic was also shown to be suitable as a resin for stereolithography 3D printing on a benchtop printer through the inclusion of a RAFT agent, achieving semi-IPN printed objects in a two-step approach.
One of the most popular combinations pursued in the design of orthogonal polymerization systems is the combination of radical polymerization (either free-radical or reversible-deactivation radical polymerization) and ring opening polymerization (ROP), to realise a variety of polymer architectures including block9–16 and graft17–19 copolymers. In the case of block copolymers, orthogonal polymerization of a vinyl monomer and a lactone is most typically achieved using a bi-functional initiator or catalyst. Some specific examples have been demonstrated, such as using the nitroxide-mediated polymerization of styrene and ROP of ε-caprolactone (CL),10 atom transfer radical polymerization (ATRP) of various acrylates and methacrylates combined with the ROP of CL and lactide,11,16 and the reversible addition–fragmentation chain transfer (RAFT) polymerization of N-isopropylacrylamide (NIPAM) in combination with the ROP of lactide.12 These processes were typically performed at elevated temperatures, under oxygen-free conditions, to generate the targeted block or graft copolymers.
More recently, there has been a shift towards enabling polymerization processes that yield complex morphologies to proceed under relatively benign reaction conditions, including in the presence of air. Yu et al.13 demonstrated the RAFT block copolymer synthesis of CL and N-vinylcaprolactam (as well as N-vinylcaprolactam/N-vinylpyrrolidone copolymers) at 30 °C in air, through the strategic choice of initiator and catalyst for both the radical and ring opening polymerization steps. Villarroya et al.14 performed simultaneous ATRP and enzymatically mediated ROP of methyl methacrylate (MMA)/2-hydroxyethyl methacrylate with CL to generate block-graft copolymers, this time in supercritical carbon dioxide under relatively mild reaction temperatures (35 °C). The advent of photoinduced electron/energy transfer RAFT (PET-RAFT) polymerization, as developed by Boyer's group,20–22 has further continued this trend by utilising the energy from visible or UV light to facilitate radical polymerization in a controlled fashion. Their group has demonstrated orthogonal block copolymerization of CL with methyl acrylate under ambient conditions, either in a sequential or simultaneous fashion, through the use of blue light and an iridium(III) photocatalyst (for PET-RAFT) and diphenyl phosphate (DPP) as ROP catalyst.23 In a similar vein, visible-light driven photoacid generation to catalyse ROP of CL in an orthogonal manner to PET-RAFT polymerization was reported by the same authors.24
The above-mentioned examples of preparing complex polymer architectures are all based on polymerization methods in an appropriate solvent (typically an organic solvent) for both blocks or resulting polymeric phases. However as noted by Reese et al.,2 there is a desire in many materials applications to perform polymerizations in neat or solventless conditions – for example to reduce harmful byproducts and chemical waste, or enabling the transformation of a liquid monomeric resin into a solid polymer of particular shape, such as in the case of 3D printing technologies. With respect to replacing traditional and potentially harmful solvents, deep eutectic solvents (DESs)25–27 represent an exciting class of mixtures that have shown potential to act as powerful solvents in chemical synthesis, as well as separation science,28,29 energy storage,30,31 and biotechnology,32 amongst others. DESs are most typically binary mixtures of hydrogen bond donating and accepting compounds, forming a mixture with significantly lower melting point than either starting material.33 The interpretation of what is a DES remains an important debate, with a mixture where favourable interactions between components result in enthalpic-driven negative deviations from ideal mixing a preferred general definition.34 With advantageous physical and chemical properties including low volatility, tuneable chemical composition and viscosity, low flammability and potential to be recycled and recovered, DESs have been used extensively to prepare materials such as polymeric gels (“eutectogels”),35 monoliths36,37 and molecularly imprinted polymers.38–43 When one or more component of the DES is polymerizable, which we term “polymerizable eutectics” (PEs),44,45 the solvent-free polymerization of these mixtures is readily achieved. This has been demonstrated in the context of photocured eutectogels,46–48 frontal polymerization,49–52 and various types of 3D printing technologies.53–56 Our group has also recently shown the synthesis of block copolymers prepared directly from a PE based on NIPAM and CL, in essence a solvent-free block copolymerization using a bifunctional RAFT agent.57
Recent advances in the design of PEs based on lactones for ROP,58–60 as well as PEs consisting of monomers polymerizable via different mechanisms, inspired us to design and prepare PE-based interpenetrated polymer networks through a combination of radical and ring opening polymerizations. Interpenetrating polymer networks (IPNs) are systems that consist of two crosslinked polymer networks which are physically entangled but not chemically connected to each other;61 the mechanical properties and swelling behaviour of IPNs is typically highly distinct in comparison to single networks.62 IPNs (or semi-IPNs, whereby one cross-linked network is physically entangled with a linear polymer) are most typically prepared by a (i) sequential method where a single network is swollen with a second monomer and cross-linker, then polymerized, or (ii) a simultaneous method, requiring orthogonal polymerization chemistry. Various IPNs or semi-IPNs incorporating poly(ε-caprolactone) (PCL) have been reported,63–66 however these are almost always prepared sequentially, and from either linear or multi-arm PCL architectures. Herein, we demonstrate the first synthesis of IPNs and semi-IPNs based on PEs composed of a vinyl monomer (NIPAM) and a lactone (CL) to facilitate orthogonal polymerization. PNIPAM is a well-known thermoresponsive polymer,67 enabling the design of stimuli-responsive polymer networks, whilst polyesters such as PCL are readily amenable to chemical degradation (e.g. via hydrolysis) and can be cross-linked through the inclusion of appropriate bis(carbonate) or bis(lactone) cross-linkers.68 Through cross-linking one or both phases, we demonstrate the solvent-free, one-pot synthesis of network polymers with unique polymer topologies and swelling capacity. These PEs are further demonstrated in the context of stereolithography 3D printing on a commercially available benchtop printer.
:
CL0.67 PE, followed by irradiation and/or thermal polymerization in ambient air in a closed vial. NIPAM polymerization was initiated by irradiation of TPO with a UV lamp (SUN 54 W UV LED lamp, λmax = 370 nm) for up to 5 minutes. A stock solution was prepared of TPO in DMF (0.01 g mL−1) and this solution was pipetted directly into PE mixtures prior to irradiation to achieve an initial ratio of [NIPAM]
:
[TPO] of 100
:
0.08. CL polymerization was catalysed by TEHA or MSA, each with BnOH as an initiator. TEHA-catalysed experiments were carried out at 90 °C, and the initial ratio of [CL]
:
[BnOH]
:
[TEHA] was 200
:
5
:
5, while MSA-catalysed experiments were performed at room temperature (20–23 °C) where the initial ratio of [CL]
:
[BnOH]
:
[MSA] was 200
:
5
:
10. For sequential polymerization experiments where NIPAM was polymerized first, all reagents were added to the PE prior to UV irradiation except TEHA or MSA. For simultaneous and sequential experiments where CL was polymerized first, all reagents were added at the beginning.
Homopolymer control experiments were carried out with the reagent ratios listed above for NIPAM (either using DMSO as a solvent or in a NIPAM-CL0.67 eutectic mixture), and for CL (neat CL, with DMSO as a solvent, or in a NIPAM-CL0.67 eutectic mixture). For experiments with monomer dissolved in DMSO the mass fraction of the monomer was equivalent to the NIPAM
:
CL0.67 eutectic mixtures. Linear homopolymers and polymer blends were isolated for analysis by precipitation from THF to hexanes.
:
1. For CL crosslinking with TEHA, approximately 0.3 g of reaction mixture was placed in a glass vial (11 mm internal diameter) which was degassed with N2 for 10 minutes prior to heating at 90 °C in an oil bath overnight. For NIPAM crosslinking approximately 0.3 g of reaction mixture was placed in a rectangular mould (flat embedding PTFE mould with metal frame from Ted Pella Inc. Cavity dimensions: 14 × 6.9 × 3 mm) and the sample was irradiated with a UV lamp (370 nm) for 2 minutes on each side open to air. Interpenetrating polymer networks (IPNs) were prepared sequentially by adding all initiators, catalysts and crosslinkers to the NIPAM-CL0.67 mixture in a closed glass vial and then either exposing to UV light in air first (reaction (1), PNIPAMx-PCLx), or degassing and heating first (reaction (2), PCLx-PNIPAMx), followed by the other treatment. Semi-IPN samples were prepared by first polymerising CL with MSA in the PTFE mould open to air, followed by UV irradiation open to air (2 min on each side) to crosslink the NIPAM (PCL-PNIPAMx).
Mixed-mode PE resins were prepared following the protocol above, with the addition of Zn(OAc)2 in the resin (initial ratio of [CL]
:
[Zn(OAc)2] = 200
:
1) to achieve semi-IPNs via 3D printing. 3D printing of hollow cubes was carried out with the following parameters: bottom layer exposure time = 15 s, regular layer exposure time = 12 s, with all other parameters as listed above. After printing the material was placed in a sealed glass vial and heated to 100 °C in air overnight for polymerization of CL resulting in PNIPAMx-PCL semi-IPNs.
944
000 g mol−1.
:
lactone, to construct a binary solid–liquid equilibrium (SLE) phase diagram of melting point(s) as a function of composition. Compositions that were stable liquids at room temperature were targeted for subsequent polymerization. Upon visual inspection of the mixtures upon heating and stirring then cooling to room temperature, stable liquids formed for all compositions xCL > 0.5 and xVL > 0.5 (Fig. 1A). Stable mixtures can also be prepared at low NIPAM/high lactone mole fractions at room temperature without the need for heating, however for consistency we retain a heating and stirring protocol for all mixtures in this work.
![]() | ||
| Fig. 1 (A) Photo of NIPAM-CL eutectic mixtures with the CL mole fraction listed below each vial. (B) NIPAM-CL phase diagram showing experimental onset melting temperatures as well as ideal melting points calculated using eqn (1). All error bars are smaller than the symbol size (n = 2). The dotted line represents approximate room temperature. (C) TGA thermograms of monomers and NIPAM-CL0.67 eutectic mixture. | ||
When constructing a binary SLE phase diagram, experimental melting points can be compared to the melting point depression predicted by the isobaric mixing of two pure compounds, namely:34,70
![]() | (1) |
:
2 choline chloride
:
ethylene glycol mixture) exhibiting close to ideal phase behaviour.73 The terms “eutectic solvents”35 or “low transition temperature mixtures”26 are recommended by some researchers, with the most important aspect being that these are functional supramolecular liquids with unique physical and chemical properties.
Differential scanning calorimetry (DSC) was used to quantify enthalpies of fusion of our starting materials, as well as the melting point onset of our mixtures. We use the melt onset from heating loops to construct binary SLE diagrams (Fig. 1B), given that a reasonably significant freezing point hysteresis was observed in the cooling loops regardless of scan rate (see Fig. S2, ESI†), which may be in part due to a supercooling effect under DSC conditions.74,75 For our pure compounds, excellent agreement with literature melting points was found when using the melt onset, justifying our choice. The SLE phase diagram is shown in Fig. 1B along with the predicted liquidus line assuming ideality, which was determined from eqn (1) using experimental data for pure compounds (NIPAM: ΔfusH = 15 526 J mol−1, m.p. = 337.95 K; CL: ΔfusH = 11
272 J mol−1, m.p. = 261.15 K). We observe two melting transitions for all compositions where xCL < 0.75, where the first melt (blue squares) is attributed to the solidus line of the phase diagram. The average temperature of the first melt (264 ± 2 K) is close to the predicted ideal eutectic temperature (258.3 K), supporting the notion that these mixtures exhibit near-to-ideal mixing. Similar behaviour is observed for NIPAM-VL mixtures (see Fig. S3 & S4, ESI†). Targeting a polymerizable eutectic that is both a stable room temperature liquid and a relatively high proportion of each monomer for subsequent polymerization, the composition xCL = 0.67 was chosen for further analysis. Thermal stability of this mixture (purple line, Fig. 1C) as determined by TGA was shown to exhibit characteristics of both components; the maximum decomposition temperature was similar to that of NIPAM, with a residual mass at higher temperatures similar to that of CL.
The NIPAM-CL0.67 PE was characterized by 1D and 2D NMR spectroscopy following the same protocol as previous reports.48,57,76 A high degree of association was present in these mixtures as evidenced through 1D and 2D 1H NMR spectroscopic measurements; the 1D spectrum exhibits broader resonances that are shifted downfield relative to the pure starting materials (Fig. 2D). 1H-1H ROESY data demonstrate a number of off-diagonal cross-peaks that are consistent with close association of the two PE components through space (Fig. 2E). There are distinct correlations between the vinyl protons of NIPAM and the β and γ protons in CL and these signals have been identified with black boxes in Fig. 2E. 2D DOSY NMR measurements (Fig. S5, ESI†) indicate a separate diffusion coefficient for each monomer in the PE (approximately 10−10.0 m2 s−1 for NIPAM and 10−9.8 m2 s−1 for CL). We have previously shown that the self-diffusion coefficient for NIPAM in water is ∼10−9.1 m2 s−1,76 demonstrating that the monomers in our PE have significantly reduced mobilities compared to those in a conventional solvent. The viscosity of the NIPAM-CL0.67 PE was measured to be 8.5 cP at 25 °C, similar to previously reported acrylate and acrylamide-based PEs.48,57 PCL as an impurity is sometimes observed in the PE mixtures at low concentrations (5 mol% relative to total CL) prior to the addition of ROP catalysts, which we also see by DOSY NMR (see Fig. S5, ESI†).
:
CL PEs where xCL = 0.67. These reactions were carried out in the absence of cross-linkers, to fully characterise the linear polymers formed. NIPAM was polymerized using TPO as a UV-active Type I photoinitiator upon exposure to 370 nm UV light; CL was polymerized via one of two common ROP catalysts, namely methanesulfonic acid (MSA) at room temperature, or tin(II) 2-ethylhexanoate (TEHA) at 90 °C, each using benzyl alcohol (BnOH) as an initiator. These processes are shown in Scheme 1A.
We commenced by performing control experiments where either NIPAM or CL was polymerized, either in the as-prepared PE or, as comparison, in the bulk or a traditional solvent at the same mass fraction of monomer. The results are shown in Fig. 3. The photopolymerization of NIPAM in the PE is rapid, achieving a conversion of ∼65% in 2 minutes (red triangles, Fig. 3A). The reaction proceeds at a comparable rate and final conversion to that performed in DMSO (green squares), and the polymerization is not inhibited by the presence of TEHA catalyst for the ROP process. The ROP of CL was examined in neat CL, solution (DMSO) and eutectic polymerization via two catalysts (Fig. 3B and C). As anticipated due to the higher monomer concentration, the neat polymerization of CL was the fastest process. Encouragingly, the polymerization was much faster in the PE compared to in DMSO, for both sets of catalysts studied, with quantitative conversion of monomer to polymer. Our group has observed similar increases in reaction rates previously, which we attribute to both the higher viscosity of PEs compared to traditional solvents, which decreases the rate of chain stoppage events in the reaction medium.57,76 A small increase in polymerization rate at low conversion/early time is observed for the TEHA catalyzed polymerization of CL in the presence of TPO (red triangles and purple diamonds, Fig. 3B), the mechanistic origins of which are unclear at this point.
![]() | ||
| Fig. 3 Homopolymer control experiment conversion data for (A) NIPAM initiated by TPO, (B) CL catalysed by TEHA and (C) CL catalysed by MSA. | ||
Various orthogonal polymerizations of our PEs were then performed according to the reaction pathways described in Scheme 1B. For Reaction 1 the ROP catalyst was added to the PE mixture after polymerization of NIPAM, while for reaction (2) and (3) all initiators and catalysts were present in the PE mixture prior to any polymerization. Fig. S6C (ESI†) shows representative 1H NMR spectra with integration regions used to calculate monomer conversion. In order to calculate conversion when both polymers are present, the integration of the PCL peak at 2.30 ppm is subtracted from the integration of the overlapping PNIPAM and PCL signals at 4.00 ppm to determine the PNIPAM signal area. When NIPAM is polymerized first, followed by CL using TEHA as catalyst at 90 °C (Fig. 4A), PNIPAM is formed very quickly in the timescale of the reaction, and to a comparable conversion to the data in Fig. 3A. The presence of linear PNIPAM and the corresponding increase in sample viscosity does not impede the full conversion of CL over 24 h. In the reverse process (CL first followed by NIPAM, Fig. 4B), the polymerization of CL proceeds smoothly to full conversion in 6 h, with zero conversion of NIPAM (even at the elevated reaction temperature of 90 °C). After polymerization of CL, the reaction mixture becomes slightly opaque, however this does not affect the next step; upon irradiation with UV light, the conversion of NIPAM is essentially quantitative over a few minutes. The simultaneous polymerization (Fig. 4C) is ‘the best of both worlds’, with rapid conversion of NIPAM and rapid polymerization of CL, achieving >80% conversion in 5 hours. The use of MSA as catalyst at room temperature (Fig. 4D–F) gives inferior results in some instances – when CL is polymerized last, or sequentially (Fig. 4D and F), the conversion is much lower compared to the use of TEHA. This is attributed to the lower reaction temperature (90 °C vs. room temperature), which greatly influences the reaction viscosity (in particular, when a high mass fraction of PNIPAM is present). We subsequently focus on the TEHA catalysed systems due to the high conversion of both monomers, however room temperature reactions can be advantageous in numerous instances, which we discuss later in the manuscript.
Linear homopolymers and polymer blends were isolated by precipitation and were analysed via TGA and GPC. Select TGA thermograms and GPC chromatograms are displayed in Fig. 5 comparing PNIPAM and PCL homopolymers each prepared from a eutectic mixture, with PNIPAM-PCL polymer blends prepared via reaction (3) (the simultaneous pathway). TGA thermograms and GPC chromatograms for all samples in this work are shown in Fig. S7 and S8,† respectively, and summarised in Table 1. Homopolymer control experiments for both PNIPAM and PCL show that both the molar mass distribution and the mass loss profile by TGA are comparable between reactions performed in the eutectic and those performed either in the bulk or in DMSO; the polymers have comparable molar mass distributions with relative Mn values between 3–7 kDa; given the high initiator loading these molar mass distributions are not unexpected. The thermal stability and number average molar mass for PCL is higher when MSA is used as a catalyst compared to TEHA (see entries 3–5 & 6–8, Table 1); the value of Tmax increases by close to 100 °C when MSA is used, which is attributed to the differing end-groups as a result of the choice of catalyst influencing the thermal stability of the polymer.77 The TGA profile of our simultaneous polymerization (using TPO/TEHA, entry 11, Table 1; Fig. 5A, central panel) has distinct features with a two-step mass loss profile that can be directly attributed to PCL and PNIPAM respectively. Assuming the mass change in each section of the TGA profile corresponds to homopolymer decomposition of either PNIPAM or PCL, the PCL mass fraction in each system was 0.72, 0.72 and 0.76 (for reaction (1), reaction (2) and reaction (3) respectively), which is in good agreement with the mass fraction of the original composition of the eutectic.
| Entry # | Sample | Initiator/catalyst | T max (°C) |
M
n a (g mol−1) |
Đ |
|---|---|---|---|---|---|
| a Relative to PMMA standards by THF GPC. | |||||
| 1 | PNIPAM-DMSO | TPO | 414.1 | 3930 | 1.5 |
| 2 | PNIPAM-CL | TPO | 405.4 | 3280 | 1.6 |
| 3 | PCL neat | TEHA | 309.5 | 4390 | 1.4 |
| 4 | PCL-DMSO | TEHA | 308.4 | 3870 | 1.4 |
| 5 | PCL-NIPAM | TEHA | 318.1 | 3520 | 1.4 |
| 6 | PCL neat | MSA | 407.3 | 7260 | 1.9 |
| 7 | PCL-DMSO | MSA | 405.0 | 4140 | 1.6 |
| 8 | PCL-NIPAM | MSA | 405.6 | 6950 | 1.4 |
| 9 | PNIPAM-PCL R1 | TPO/TEHA | 314.5 | 3620 | 1.2 |
| 10 | PNIPAM-PCL R2 | TPO/TEHA | 321.8 | 3300 | 1.5 |
| 11 | PNIPAM-PCL R3 | TPO/TEHA | 316.7 | 3720 | 1.5 |
| 12 | PNIPAM-PCL R1 | TPO/MSA | 380.8 | 2880 | 1.1 |
| 13 | PNIPAM-PCL R2 | TPO/MSA | 397.7 | 3410 | 1.2 |
| 14 | PNIPAM-PCL R3 | TPO/MSA | 371.7 | 3150 | 1.2 |
![]() | ||
| Fig. 6 (A) Scheme showing the sequential preparation of PNIPAMx & PCLx IPNs. Reactions A and B have the same conditions as in Scheme 1A with the addition of PEGDA for reaction (A), and bis(carbonate) for reaction (B). PCL-PNIPAMx semi-IPNs were prepared following reaction (2) without bis(carbonate) crosslinker present. (B) TGA thermograms of IPNs. | ||
Initially, cross-linked PNIPAM and PCL homopolymer gels were prepared from both PEs and a conventional solvent (DMSO), as well as in the bulk for CL for comparison. PNIPAMx-DMSO gels were optically transparent, while PNIPAMx-CL gels prepared under the same conditions were opaque (Fig. S9A, ESI†). All PCL gels (PCLx neat, PCLx-DMSO, PCLx-NIPAM) were opaque with a slight yellow colour due to the bis(carbonate) crosslinker (Fig. S9B, ESI†). PCLx-NIPAM gels were better at retaining their original shape after washing and drying compared with PCLx neat or PCLx-DMSO. To evaluate their level of cross-linking, the swelling of dried homopolymer gels was studied in water (for PNIPAMx) and chloroform (for PCLx). This data is shown in Table 2. The swelling ratio of PCL networks in chloroform had a large standard deviation compared with swelling in water due to the rapid evaporation of chloroform from these samples. Additionally, PCLx neat samples lacked structural integrity after swelling and some samples crumbled into several pieces. PNIPAMx gels showed reversible thermoresponsive swelling in water (Table 2, entries 1 and 2), as anticipated due to the lower critical solution temperature (LCST) of PNIPAM at ∼32 °C, resulting in a volume phase transition temperature (VPTT) of these networks. The swelling ratio of PNIPAMx is similar when prepared either in DMSO or in CL, indicating a comparable level of cross-linking. The effective cross-link density qeff of these networks was estimated via Flory–Rehner theory78 (see ESI† and Table 2). PCLx essentially undergoes no swelling in water (entries 3–5), but swells substantially in chloroform; the gel prepared from the PE (entry 5) has the lowest cross-link density and highest swelling capacity. Notably, the cross-link density of the PCL networks is significantly lower than the predicted value (qpredeff = 0.1, based on 5 mol% of cross-linker in the mixture and 2 cross-link sites formed per molecule), suggesting a relatively low fraction of the bis(carbonate) crosslinker incorporated into the network structure.
| Entry # | Sample | S water (RT) | S water (45 °C) | S CHCl3 | q eff |
|---|---|---|---|---|---|
| a Denotes sample crumbled when immersed in solvent. RT = 20–23 °C. n = 2 for all samples except those denoted *n = 3, ^n = 1. | |||||
| 1 | PNIPAMx-DMSO | 2.29 ± 0.04* | 0.40 ± 0.03* | x | 0.17 |
| 2 | PNIPAMx-CL | 2.14 ± 0.07* | 0.37 ± 0.01* | x | 0.19 |
| 3 | PCLx bulk | 0.04 ± 0.01 | — | 8.31 ± 0.02 | 0.01 |
| 4 | PCLx-DMSO | 0.041 ± 0.008 | — | 12.7 ± 0.9 | 0.005 |
| 5 | PCLx-NIPAM | 0.044 ± 0.006 | — | 15.2 ± 0.2 | 0.004 |
| 6 | PNIPAMx-PCLx R1 IPN | 1.44^ | 0.25^ | 3.74^ | |
| 7 | PCLx-PNIPAMx R2 IPN | x | — | — | |
| 8 | PCL-PNIPAMx semi-IPN | 1.95 ± 0.01 | 0.3 ± 0.1 | — | |
IPNs were subsequently prepared from our PEs using two sequential one-pot approaches, where either NIPAM (reaction(1)) or CL (reaction (2)) was the first phase to be cross-linked (entries 6, 7, Table 2 and Fig. 6B). While the conversion of CL with TEHA was similar regardless of reaction order for linear polymerization (Fig. 4A and C), the relative mass fraction PNIPAMx and PCLx in the resulting IPNs based on TGA data was dependent on the order of cross-linking (Table S1, ESI†). The behaviour of these networks in water and chloroform was also studied. When PCL was cross-linked first followed by PNIPAM (rection (2), entry 7), the network lacked the structural integrity to remain intact when immersed in water. In comparison, PNIPAM crosslinking followed by PCL worked well (reaction (1), entry 6), forming a robust IPN. The network showed thermoresponsive swelling in water as well as swelling in chloroform, however the equilibrium swelling capacity in each solvent was reduced compared to homopolymer gels. This is attributed to both the inter-entanglement of cross-linked PCL and PNIPAM domains within the IPN and unfavourable polymer-solvent interactions (e.g. PCLx and water) that favour a contraction of the network. Semi-IPNs were also successfully prepared (reaction (2), entry 8) where linear PCL was first formed, followed by polymerization and cross-linking of NIPAM resulting in a semi-2 type IPN (linear polymer prepared first, followed by a crosslinked network).79 For this process CL was polymerized in situ using MSA as catalyst in air at room temperature, enabling the entire process to be performed in an open PTFE mould with no complicated equipment (see Fig. S11, ESI†). PCL-PNIPAMx semi-IPNs were washed with water and then chloroform to remove any unreacted monomer and linear PCL before drying; the thermoresponsive swelling capacity of this PNIPAMx network in water was reduced in comparison to homopolymer PNIPAM networks prepared in the absence of PCL.
Similar to our bulk cured networks, these printed objects possess thermoresponsive behaviour when immersed in water. At room temperature, the object symmetrically swells to approximately 1.5 times its original external size, with a significant increase in mass due to absorbed water, and loss of optical transparency, whilst retaining its structural features (see Table S2,† and Fig. 7, bottom right panel). When the swollen object is heated through the LCST of PNIPAM to 45 °C, we observe mass loss due to desorbed water, coupled with only a very small decreased in external size as well as loss of the smooth structural features of the original cube. A rough, “ragged/buckled” cube is formed as a result, which is fully reversible back to the “ordered” structure when allowed to cool back to room temperature in water. This observation could be attributed to the buckling of the PNIPAM network due to the osmotic pressure created as water desorbs from the outermost surface of the printed object at higher temperatures.81
As a final investigation of orthogonal preparation of IPNs from PEs, we prepared 3D printing PE resins also containing the reagents required for subsequent CL polymerization. This enables the preparation of semi-1 IPNs where linear PCL is formed within a PNIPAMx 3D-printed network. For these printing experiments the same base resin formulation was used as for the NIPAM-only polymerization discussed above. Initial attempts where TEHA was incorporated into the resin resulted in unsuccessful printing, attributed to unwanted formation of linear PCL during the print step. This altered the viscosity of the resin and required UV exposure to achieve sufficient curing throughout each layer of the print. While the linear polymerization of NIPAM and CL with TPO and TEHA was orthogonal under 370 nm irradiation (Fig. 4), this orthogonality was lost when using the different wavelength of the 3D printer (λmax = 405 nm). An alternative ROP catalyst, zinc acetate,82 was subsequently used which resulted in successful printing of PNIPAMx structures from the PE resin containing CL and zinc acetate throughout the material (Fig. 7B). This structure was placed in a sealed glass vial and heated at 100 °C to polymerize the CL; as a visual indication of PCL formation, the opacity of the material increased after heat treatment. These semi-IPN materials were studied via TGA after each step to determine the relative mass fractions of each component. Fig. 7C shows the TGA thermograms after 3D-printing, prior to ROP of CL (PNIPAMx-CL (Zn(OAc)2)) as well as after heating the material to polymerize CL (PNIPAMx-PCL semi-IPN). The as-printed material shows a significant mass loss (64.9%) around 144 °C. This is in excellent agreement with the initial mass fraction of CL in the resin (65.5%), supporting minimal PCL formation during the printing process. After heating, this first mass loss (135 °C) was greatly reduced (17% of total mass). This result indicates that a considerable amount of CL is polymerized within the PNIPAMx network structure, yielding a PNIPAMx-PCL 3D-printed semi-IPN.
Raw data for this manuscript (graphical outputs of processed DSC traces, raw mass vs. temperature data for TGA thermograms, RI signal vs. time, Mw calculated from PMMA standards for GPC elution data, 1H NMR spectra, tabulated conversion-time data from polymerizations, and .ctb slice files for 3D printing) are publicly available at the University of Tasmania Research Data Portal (https://www.rdp.utas.edu.au) and accessible at the following address: https://dx.doi.org/10.25959/18hy-nb80.
den
Bruinhorst and M. C. Kroon, Angew. Chem., Int. Ed., 2013, 52, 3074–3085 CrossRef CAS PubMed.Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4py01456a |
| This journal is © The Royal Society of Chemistry 2025 |