Oliver J.
Deane
,
James
Jennings
and
Steven P.
Armes
*
Dainton Building, Department of Chemistry, University of Sheffield, Brook Hill, Sheffield, South Yorkshire S3 7HF, UK. E-mail: s.p.armes@sheffield.ac.uk
First published on 7th October 2021
2-Hydroxypropyl methacrylate (HPMA) is a useful model monomer for understanding aqueous dispersion polymerization. 4-Hydroxybutyl acrylate (HBA) is an isomer of HPMA: it has appreciably higher aqueous solubility so its homopolymer is more weakly hydrophobic. Moreover, PHBA possesses a significantly lower glass transition temperature than PHPMA, which ensures greater chain mobility. The reversible addition–fragmentation chain transfer (RAFT) aqueous dispersion polymerization of HBA using a poly(ethylene glycol) (PEG113) precursor at 30 °C produces PEG113–PHBA200–700 diblock copolymer nano-objects. Using glutaraldehyde to crosslink the PHBA chains allows TEM studies, which reveal the formation of spheres, worms or vesicles under appropriate conditions. Interestingly, the partially hydrated highly mobile PHBA block enabled linear PEG113–PHBAx spheres, worms or vesicles to be reconstituted from freeze-dried powders on addition of water at 20 °C. Moreover, variable temperature 1H NMR studies indicated that the apparent degree of hydration of the PHBA block increases from 5% to 80% on heating from 0 °C to 60 °C indicating uniform plasticization. In contrast, the PHPMAx chains within PEG113–PHPMAx nano-objects become dehydrated on raising the temperature: this qualitative difference is highly counter-intuitive given that PHBA and PHPMA are isomers. The greater (partial) hydration of the PHBA block at higher temperature drives the morphological evolution of PEG113–PHBA260 spheres to form worms or vesicles, as judged by oscillatory rheology, dynamic light scattering, small-angle X-ray scattering and TEM studies. Finally, a variable temperature phase diagram is constructed for 15% w/w aqueous dispersions of eight PEG113–PHBA200–700 diblock copolymers. Notably, PEG113–PHBA350 can switch reversibly from spheres to worms to vesicles to lamellae during a thermal cycle.
Fig. 1 Chemical structures for (a) 2-hydroxypropyl methacrylate (HPMA; only the major isomer is shown in this case) and (b) its acrylic isomer, 4-hydroxybutyl acrylate (HBA). |
Essentially, the HPMA repeat units nearest the block junction become hydrated, which leads to a shift in the effective block junction. This is sufficient to lower the fractional packing parameter P from the relatively narrow range that favors worms (0.33 < P ≤ 0.50) to that corresponding to spheres (P ≤ 0.33). Importantly, this morphological transition proved to be reversible, which has enabled various cell biology studies to be explored for worm gels.7,32,55,56 Similarly, macromolecular RAFT agents based on monomethoxy-capped poly(ethylene glycol) (PEG) have been used by various research groups to design thermoresponsive PEG–PHPMA nano-objects.52,53,57,58 More specifically, esterification enables the synthesis of well-defined PEG precursors with minimal batch-to-batch variation.52,53,56–58 Furthermore, using PEG as a steric stabilizer ensures well-resolved proton signals for each block, which in turn should facilitate variable temperature 1H NMR spectroscopy studies.
In principle, an alternative route to thermoreversible PEG-based diblock copolymer nano-objects could be achieved by employing a less hydrophobic vinyl monomer that exhibits greater thermoresponsive behavior.50,59 Recently, Byard et al. reported the one-pot PISA synthesis of poly(N,N-dimethylacrylamide)–poly(4-hydroxybutyl acrylate-stat-diacetone acrylamide) [PDMAC56–P(HBA-stat-DAAM)264].50 This amphiphilic diblock copolymer exhibited remarkable self-assembly behavior, with thermoreversible transitions between spheres, worms, vesicles and lamellae being observed in aqueous solution for a single copolymer simply by adjusting the temperature.50 Variable temperature 1H NMR studies indicated that the weakly hydrophobic HBA repeat units became more hydrated at elevated temperatures. This seems rather counter-intuitive: precisely the opposite behavior is observed for PHPMA-based diblock copolymers, for which the HPMA repeat units become marginally less hydrated on heating.7,50 This apparent difference is particularly striking given that HPMA and HBA are structural isomers (Fig. 1). Unfortunately, the statistical copolymerization of 20 mol% DAAM comonomer with HBA by Byard et al. prevents a direct comparison of the thermoresponsive behavior of PHBA and PHPMA. This problem is resolved in the present study.
Herein we report the RAFT aqueous dispersion polymerization of HBA using a PEG113 precursor to afford thermoresponsive diblock copolymer spheres, worms or vesicles at 30 °C (Scheme 1). TEM studies of such low Tg nano-objects requires chemical crosslinking of the PHBA chains via their pendent hydroxyl groups.60 Such covalent stabilization enables the construction of a pseudo-phase diagram using TEM to assign copolymer morphologies. The thermoreversible behavior of linear PEG113–PHBA260 nano-objects is assessed using oscillatory rheology, dynamic light scattering (DLS) and small-angle X-ray scattering (SAXS) and is explicitly compared to that of PEG113–PHPMA260 nano-objects. Variable temperature 1H NMR spectroscopy is used to monitor the degree of hydration of the PHBA block and the reconstitution of freeze-dried PEG113–PHBAx powders to form aqueous dispersions of diblock copolymer nano-objects at neutral pH is examined at 20 °C. Finally, a first-of-its-kind variable temperature phase diagram is constructed to highlight the copolymer morphologies that are accessible for such PEG113–PHBAx diblock copolymers.
To further examine the difference between these two PISA formulations, 15% w/w aqueous dispersions of PEG113–PHPMA260 and PEG113–PHBA260 nano-objects were prepared via RAFT aqueous dispersion polymerization at 30 °C. 1H NMR analysis confirmed that a DP of 260 was achieved in each case. DMF GPC analysis indicated similar Mn values and dispersities for PEG113–PHBA260 and PEG113–PHPMA260 (Fig. S1b†). Given the high blocking efficiencies and essentially full monomer conversions, the small difference in Mn values is attributed to a slightly larger hydrodynamic radius for PEG113–PHPMA260 chains in DMF. Visual inspection indicated that the PEG113–PHBA260 nano-objects formed a free-flowing, highly transparent fluid at 20 °C, whereas the PEG113–PHPMA260 nano-objects formed a viscous turbid fluid at the same temperature.
TEM analysis of PHPMA-based nano-objects is well established in the literature.28,34,52,61–65 Differential scanning calorimetry (DSC) studies indicated a relatively high Tg of 94 °C after drying under vacuum for three days at 30 °C (Fig. 2a, purple trace) for a PHPMA200 homopolymer, which is consistent with the literature.28 This Tg enabled high-quality TEM images to be readily obtained when using a heavy metal stain to enhance electron contrast. In contrast, the sub-ambient Tg of −23 °C indicated by DSC analysis of PHBA200 homopolymer (Fig. 2a, red trace) prevents TEM analysis of linear PEG113–PHBA260 nano-objects owing to nanoparticle deformation and/or film formation during grid preparation. Moreover, the partially hydrated nature of the PHBA chains leads to poor electron contrast when using cryo-TEM.39 Further DSC studies indicated that the Tg of PHBA has a rather weak molecular weight dependence (Fig. S2†).
Glutaraldehyde (GA) is a well-known fixative that is commonly used to crosslink biological samples such as proteins prior to TEM studies.66–69 The aqueous chemistry of GA is rather complex: depending on the solution pH, a mixture of monomeric GA, polymeric GA and cyclic GA species can be formed.70 Nevertheless, the two aldehyde groups on GA can react efficiently with adjacent hydroxy groups on poly(vinyl alcohol) (PVA).71,72 Very recently, we found that GA provides sufficient covalent stabilization of PHBA-based nano-objects to enable good-quality TEM images to be obtained.60 Moreover, by avoiding copolymerization of HBA with crosslinkable comonomers such as DAAM, this approach facilitates direct comparison of the thermoresponsive behavior of PHPMA-based and PHBA-based nano-objects.
In the present study, the [GA]/[HBA] molar ratio was systematically varied from 0.25 to 1.00 when crosslinking a 5% w/w aqueous dispersion of PEG113–PHBA260 nano-objects. Empirically, the optimum [GA]/[HBA] molar ratio was found to be 0.66, which is significantly higher than the stoichiometric ratio of 0.25 (Fig. 2b). Moreover, using more concentrated (>7.5% w/w) aqueous dispersions led to irreversible macroscopic gelation owing to inter-particle crosslinking. DSC and FT-IR spectroscopy studies were undertaken to examine the effect of GA crosslinking on the PEG113–PHBAx diblock copolymers. Initially, linear PEG113–PHBA260 and PEG113–PHPMA260 were freeze-dried to afford a tacky gum and a glassy powder, respectively. DSC studies indicated Tg values of 85 °C for PEG113–PHPMA260 and −37 °C for PEG113–PHBA260 (Fig. 2c; purple and red traces, respectively). Interestingly, the melting transition (Tm = 58 °C73) exhibited by the PEG113 precursor (Fig. 2c, blue trace) is not observed for either linear diblock copolymer. This is attributed to the ether linkages in the PEG block forming hydrogen bonds with the hydroxyl-functional PHBA or PHPMA blocks. Comparing the DSC traces obtained for the linear PEG113–PHBA260 (red trace) and GA-crosslinked PEG113–PHBA260 (green trace) confirmed that such covalent stabilization eliminates the sub-ambient Tg associated with the PHBA block. Moreover, visual inspection indicated that the crosslinked copolymers formed glassy powders rather than tacky gums. [N. B. the broad feature observed at around 58 °C in the green trace is attributed to the partially crystalline nature of the PEG block, which can no longer form H-bonds with the GA-crosslinked PHBA chains]. FT-IR studies provided further evidence for successful GA crosslinking (Fig. S3†). Spectra recorded for the freeze-dried PEG113 precursor, a linear PHBA200 homopolymer, a linear PEG113–PHBA600 diblock copolymer and a GA-crosslinked PEG113–PHBA600 diblock copolymer are consistent with the reaction of GA with (some of) the hydroxyl groups on the PHBA chains to form ether linkages (Fig. 2b).72
In summary, DSC and FT-IR studies suggest that covalent stabilization via GA crosslinking should be sufficient to enable good-quality images to be obtained via conventional TEM. Indeed, TEM studies of an aqueous dispersion of GA-crosslinked PEG113–PHBA260 nano-objects prepared at 5% w/w using a [GA]/[HBA] molar ratio of 0.66 indicated the presence of mainly spheres with minor populations of dimers and trimers (Fig. S4a†). In contrast, no TEM images could be obtained for the corresponding linear PEG113–PHBA260 nano-objects (data not shown). Similarly, TEM analysis of a relatively viscous dispersion of the analogous linear PEG113–PHPMA260 nano-objects indicated the presence of short worms with a mean aspect (length/width) ratio of 6–7 (Fig. S4b†). This subtle difference in copolymer morphology suggests that the PHBA block is less hydrophobic than the equivalent PHPMA chains of the same mean DP. Thus, a higher PHBA DP is required to achieve the same copolymer morphology.
Two series of PEG113–PHPMA100–700 and PEG113–PHBA150–700 nano-objects were prepared by RAFT dispersion polymerization at 30 °C to enable the copolymer morphology to be directly compared at a given mean DP for the hydrophobic (meth)acrylic block. The PEG113–PHBA100–700 nano-objects were then crosslinked using GA under the optimized conditions established above. TEM studies of these two copolymer series confirmed that spheres, worms and vesicles could be obtained in both cases, with the less hydrophobic PHBA-based nano-objects typically requiring marginally higher DPs to cross each phase boundary (Fig. 3).
In particular, significantly higher PHBA DPs had to be targeted to form spheres (PHBA DP = 150–200 compared to PHPMA DP = 100–150), which is consistent with the kinetic studies (Fig. S5†). Interestingly, worms were obtained at the same structure-directing DP (DP = 300). However, the more weakly hydrophobic PHBA block provided access to a pure worm phase up to a DP of 400, whereas the corresponding PEG113–PHPMA400 only produced a mixture of worms and vesicles (Fig. 3). Moreover, pure vesicles were obtained when the PHBA DP was increased up to 500.
Warren et al. reported the formation of PEG113–PHPMA260 vesicles at 15% w/w solids, rather than the weakly anisotropic PEG113–PHPMA260 worms shown in Fig. S4b.†52 However, the former PISA syntheses were conducted at 50 °C, whereas the latter worms were prepared at 30 °C and it is well known that the precise reaction conditions can significantly influence the final copolymer morphology for this aqueous PISA formulation.38,52 Given the numerous studies and various potential applications for thermoresponsive PHPMA-based (and other structure-directing block)74 nano-objects already reported in the literature,75–77 the current study is focused on understanding the thermoresponsive behavior exhibited by the new PHBA-based nano-objects. Accordingly, a pseudo-phase diagram was constructed for a series of PEG113–PHBAx nano-objects prepared at 10–20% w/w solids via RAFT aqueous dispersion polymerization of HBA at 30 °C (Fig. 4a). GA crosslinking of the PHBA chains under optimized conditions enabled good-quality TEM images to be obtained (Fig. 4b).
Fig. 4 (a) Pseudo-phase diagram constructed for a series of PEG113–PHBAx nano-objects synthesized via RAFT aqueous dispersion polymerization of HBA at 10%, 15% or 20% w/w solids based on a combination of TEM and DLS studies conducted at 20 °C (see Table S1† for the corresponding DLS data). S + W and W + V refer to sphere plus worm and worm plus vesicle mixed phases, respectively. (b) Representative TEM images recorded for a series of GA-crosslinked PEG113–PHBAx nano-objects after GA crosslinking at 20 °C using a [GA]/[HBA] molar ratio of 0.66. (c) Selected SAXS patterns (black, blue and red symbols) and corresponding data fits (solid white lines) obtained for 1.0% w/w aqueous copolymer dispersions of linear PEG113–PHBA200 spheres, PEG113–PHBA350 worms and PEG113–PHBA600 vesicles at 20 °C and pH 7. See Table S1† for a summary of the nano-object dimensions calculated using the appropriate scattering models.80,81 |
For the PDMAC56–P(HBA-stat-DAAM)264 nano-objects recently reported by Byard et al.,50 the terminal carboxylic acid group located on the PDMAC steric stabilizer chains meant that the solution pH had to be kept relatively low (pH 3) both before and after the PISA synthesis in order to suppress end-group ionization, otherwise only kinetically-trapped spheres were obtained.78 In contrast, the non-ionic nature of the PEG113 stabilizer block employed in the current study enabled the solution pH to be adjusted up to pH 8 without generating kinetically-trapped spheres, as confirmed by DLS and aqueous electrophoresis studies (Fig. S6†).
Fig. 4c shows the X-ray scattering intensity, I(q), plotted as a function of the scattering vector, q, for 1.0% w/w aqueous dispersions of linear PEG113–PHBA200 (blue symbols), PEG113–PHBA350 (purple symbols) and PEG113–PHBA500 (red symbols) nano-objects at 20 °C and pH 7. Unlike TEM, these SAXS data are averaged over many millions of nanoparticles so they are much more statistically reliable. Moreover, GA crosslinking is not required to stabilize the copolymer morphology prior to SAXS studies. The SAXS pattern recorded for PEG113–PHBA200 nano-objects (Fig. 4c, blue symbols) had a low q gradient close to zero, which is characteristic of spheres. In contrast, the SAXS pattern recorded for PEG113–PHBA350 (purple symbols) has a low q gradient of −1, which is suggests a worm morphology.52 Finally, the SAXS pattern obtained for the PEG113–PHBA500 nano-objects (Fig. 4c, red symbols) had a low q gradient of approximately −2, which is consistent with a vesicle morphology.79 In each case, the data could be satisfactorily fitted using well-established models for the corresponding copolymer morphology. Moreover, the calculated SAXS dimensions for these linear nano-objects were consistent with TEM data, suggesting that GA crosslinking does not affect the copolymer morphology (Table S2†).80,81
Rheological studies conducted on a 15% w/w aqueous dispersion of linear PEG113–PHBA260 nano-objects indicated that a low-viscosity fluid is obtained between 10 and 30 °C (Fig. 5a). Heating this dispersion results in the formation of a soft, highly transparent, free-standing gel: the storage modulus (G′) exceeds the loss modulus (G′′) at 30–32 °C and reaches a maximum value of 20 Pa at 36 °C, which corresponds to the formation of highly linear worms with multiple inter-worm contacts.82,83 Further heating results in a significant reduction in G′ at 42 °C and a concomitant increase in solution turbidity, which is consistent with a worm-to-vesicle transition.84,85 As expected, temperature-dependent rheological studies performed on the 15% w/w aqueous dispersion of PEG113–PHPMA260 short worms confirmed no thermoresponsive behavior between 15 and 55 °C (Fig. S7†).82,86,87 The complex viscosity of the 15% w/w aqueous dispersion of linear PEG113–PHBA260 nano-objects was monitored during a thermal cycle (Fig. 5b). This data set indicated essentially no hysteresis during the sphere-to-worm and worm-to-vesicle transitions. Variable temperature DLS and SAXS studies (Fig. 5c and S8†) conducted on aqueous dispersions of linear PEG113–PHBA260 nano-objects are fully consistent with the rheology data reported in Fig. 5b (Table S3†). Moreover, SAXS analysis indicated that the solvent volume fraction (φsol) of the PHBA chains increases from 0.10 for spheres at 10 °C to 0.49 for worms at 36 °C to 0.68 for vesicles at 50 °C. Finally, the linear PEG113–PHBA300 nano-objects undergo inter-conversion between spheres, worms and vesicles over a similar temperature range (see later). In contrast, DLS data obtained for GA-crosslinked PEG113–PHBA300 worms prepared at 20 °C indicated minimal change in the sphere-equivalent hydrodynamic diameter and DLS polydispersity (see Fig. S9†), which confirms successful covalent stabilization.
It is well-documented that the shape-shifting behavior observed for certain aqueous dispersions of thermoresponsive diblock copolymer nano-objects is the result of a subtle change in the relative degree of hydration of the hydrophobic block (Scheme 2).84 For PHPMA-based nano-objects, this is believed to involve hydration of HPMA repeat units located near the block junction (surface plasticization; Scheme 2a). This has been described as an ‘LCST-like’ transition because greater (partial) hydration is observed on lowering the temperature.28,32,52,53,88,89 In contrast, HBA-rich chains appear to exhibit ‘UCST-like’ behavior.50 This simply requires that the weakly hydrophobic PHBA chains become more solvated on heating while remaining insoluble.
Variable temperature 1H NMR studies conducted between 0 and 60 °C on a 15% w/w aqueous dispersion of linear PEG113–PHBA260 nano-objects prepared in D2O yielded the spectra shown in Fig. 6. Importantly, normalizing the PEG integrals relative to those of the pyridine external standard confirmed that there was only a minimal change (ca. 5% reduction) in the degree of hydration of the PEG chains from 0 to 50 °C. Similar observations were reported for aqueous solutions of low molecular weight PEG homopolymer using ultrasonic velocity measurements.90 At 0 °C, the c′ signal is barely visible (estimated degree of hydration is ∼5%; see ESI†) but the more prominent b′ protons – which are closer to the terminal hydroxyl group – suggest a significantly higher degree of hydration of 27%. Clearly, the apparent relative degree of hydration calculated for the PHBA block depends on which proton signal is selected for analysis: proton signals arising from pendent hydrophilic groups are more prominent compared to those associated with the hydrophobic acrylic backbone.91,92 However, regardless of which proton signal is selected for quantification, the 1H NMR spectra shown in Fig. 6 indicate that the PHBA block becomes significantly more hydrated at higher temperature. This is fully consistent with the increase in φsol calculated from variable temperature SAXS experiments (Fig. S8 and Table S3†). Furthermore, variable temperature 1H NMR studies of a linear PEG113–PHBA600 confirm that no discernible hysteresis occurs during a 0 °C to 50 °C to 0 °C thermal cycle (Fig. S10†). Such changes in the (partial) degree of hydration of the PHBA block are sufficient to increase its effective volume fraction relative to that of the PEG block and hence drive an evolution in morphology from spheres to worms to vesicles as a result of the increase in the fractional packing parameter P (Scheme 2b). However, unlike the PHPMA-based nano-objects, such shape-shifting behavior must involve uniform plasticization, rather than surface plasticization.50
Fig. 6 Variable temperature 1H NMR studies of thermoresponsive linear PEG113-stabilized nano-objects dispersed in D2O (see HDO signal at 5.0–5.5 ppm in panel (c)). Chemical structures of the (a) PEG113–PHBA260 and (b) PEG113–PHPMA260 diblock copolymers with assignment of the corresponding proton signals. (b) Normalized [relative to an external standard (pyridine in 1,1,2,2-tetrachloroethane-d2) at ∼7.2 and 6.0 ppm, respectively] partial 1H NMR spectra recorded for a 15% w/w aqueous dispersion of (c) PEG113–PHBA260 and (d) PEG113–PHPMA260 nano-objects prepared in D2O on heating from 0 °C to 60 °C (N.B. the intensity of the proton signals in (d) did not change after 20 °C and are excluded for clarity). (e) Overlaid partial spectra recorded between 0 °C (blue data) and 60 °C (red data) for the four ethyl protons (b′) at 1.9–2.4 ppm within the HBA repeat units. Clearly, the PHBA block becomes more hydrated at higher temperature. (f) Overlaid partial spectra recorded between 0 °C (blue data) and 20 °C (orange data) for the pendent methyl protons (d′) at 1.3–2.0 ppm within the HPMA repeat units. The PHPMA block is only weakly hydrated at 0 °C and becomes slightly dehydrated at higher temperature. Relative degrees of hydration calculated for the hydrophobic (g) PHBA260 and (h) PHPMA260 block as a function of temperature when using proton signals a′, b′, c′ and d′. See Fig. S11† for assigned 1H NMR spectra for both PEG113–PHPMA300 and PEG113–PHBA300 diblock copolymers molecularly dissolved in CD3OD. |
Fig. 7 Variable temperature phase diagram constructed for a series of linear PEG113–PHBAx nano-objects prepared via RAFT aqueous dispersion polymerization of HBA targeting 15% w/w solids. Copolymer morphologies were initially assigned on the basis of visual appearance and corroborated by SAXS (Fig. 4c and S8†), TEM (Fig. 3, 4b and 5d) and rheological studies (Fig. 5 and S11†). [N. B. S + W, W + V and V + L denote mixed phases comprising spheres plus worms, worms plus vesicles or vesicles plus lamellae, respectively]. |
The variable temperature 1H NMR spectra recorded between 0 °C and 20 °C for a 15% aqueous dispersion of PEG113–PHPMA260 nano-objects prepared directly in DCl/D2O are shown in Fig. 6d. These spectra are consistent with the variable temperature 1H NMR spectra reported by Blanazs et al.7 and Ratcliffe and co-workers.84 However, the choice of PEG as a steric stabilizer block eliminates the problem of overlapping proton signals and so enables quantification for the first time in the present study.
More specifically, the degree of hydration of PHPMA chains is reduced from 4% to 1% on heating from 0 to 20 °C in the present study. However, further heating up to 60 °C led to no further change in the degree of hydration of the PHPMA chains.
This is in striking contrast to the monotonic increase in the (partial) degree of hydration of the PHBA chains observed over the whole temperature range for PEG113–PHBA260 nano-objects. Given that HPMA and HBA are structural isomers, it is highly counter-intuitive that their corresponding hydroxyl-functional (meth)acrylic blocks should exhibit such qualitatively different temperature-dependent hydration behavior.
Reconstitution of worm gels via redispersal of freeze-dried copolymer powder has been demonstrated for PGMA–PHPMA diblock copolymers.93 This is an important advantage for potential cell biology applications, because it means that worm gels can be readily prepared via copolymer redispersion in the cell culture medium of choice.7 TEM analysis of PEG113–PHBA200–700 nano-objects (after covalent stabilization using the GA crosslinker) confirmed that essentially the same copolymer morphology (spheres, worms or vesicles) could be obtained before and after reconstitution of an aqueous dispersion at a given temperature (Fig. S12†).
Typically, studies of thermoresponsive nano-objects focus on a single diblock copolymer composition.50,84 Here, a variable temperature phase diagram was constructed for a series of 15% w/w aqueous dispersions of PEG113–PHBAx diblock copolymer nano-objects that had been equilibrated for 2 h at 6 °C, 20 °C, 37 °C or 50 °C (Fig. 7). At 20 °C, visual inspection suggested one dispersion comprising spheres (PHBA DP = 200), two mixed sphere/worm phases (PHBA DP = 260–300), two worm dispersions (PHBA DP = 350–400), one mixed worm/vesicle phase and three vesicle dispersions (PHBA DP = 500–700). On cooling these nine aqueous dispersions to 6 °C, visual inspection indicated that the PEG113–PHBA200–350 nano-objects formed highly transparent free-flowing fluids, with DLS and TEM analysis confirming the presence of spheres. PEG113–PHBA400 formed a mixed sphere/worm phase, whereas a transparent, free-standing pure worm gel was formed by PEG113–PHBA500 (complex viscosity = 20 Pa s; Fig. S13†). For x > 500, increasingly turbid copolymer dispersions were observed, with a pure vesicle phase being obtained for PEG113–PHBA700 (Fig. 7). These copolymer dispersions were then assessed at 37 °C. The PEG113–PHBA200 spheres began to undergo a sphere-to-worm transition at this temperature but only formed a pure worm phase at 44 °C (Fig. S13†). The PEG113–PHBA260 spheres formed at 20 °C underwent 1D stochastic fusion to generate worms at 37 °C, while the PEG113–PHBA350–400 worms produced at 20 °C had evolved into vesicles at 37 °C. Finally, the PEG113–PHBA260 worm gel observed at 37 °C formed a highly turbid dispersion of pure vesicles at 50 °C (Fig. 5d) while the three examples of diblock copolymer vesicles with PHBA DPs = 350–500 were transformed into free-standing turbid pastes comprising lamellae (Fig. S14†).
In summary, PEG113–PHBAx nano-objects are clearly much more thermoresponsive than their isomeric PEG113–PHPMAx counterparts and other structure-directing blocks.42,94 This observation is expected to be important for the rational design of thermoresponsive diblock copolymer nano-objects for potential biomedical applications.
TEM studies confirmed that spheres, worms or vesicles could be obtained for both copolymer series, with the PHBA-based nano-objects typically requiring slightly higher PHBA DPs in order to produce the same nano-object morphology. Such observations are consistent with the appreciably higher aqueous solubility of HBA monomer compared to that of HPMA monomer, which implies that PHBA is more weakly hydrophobic than PHPMA.
The evolution in PEG113–PHBA260 morphology from spheres to worms to vesicles that occurred on heating proved to be highly reversible on cooling, as judged by rheology, DLS and TEM studies. In contrast, the corresponding PEG113–PHPMA260 nano-objects did not exhibit any thermoresponsive behavior, because the relatively long PHPMA block is too hydrophobic.
Variable temperature 1H NMR studies were conducted to assess the degree of hydration of the PHBA chains compared to PHPMA chains. Despite their isomeric nature, PHBA and PHPMA blocks exhibit complementary thermoresponsive behavior. Thus the PHBA chains within PEG113–PHBA260 nano-objects become significantly more hydrated on heating (from 5% at 0 °C to 85% at 60 °C), whereas PHPMA chains within PEG113–PHPMA260 nano-objects become slightly more hydrated at the lower end of the same temperature range. This remarkable difference is highly counter-intuitive and wholly unexpected: it could not be predicted from the chemical structures of HBA and HPMA. Given these 1H NMR data, the thermoresponsive behaviour exhibited by PEG113–PHBA260 nano-objects is best explained in terms of a uniform plasticization mechanism. Moreover, the relatively high chain mobility of the low Tg PHBA block is responsible for the remarkably good thermoreversibility observed for the PEG113–PHBAx nano-objects, which exhibit remarkably good thermoreversibility. Furthermore, PEG113–PHBA200–700 nano-objects can be reconstituted via direct dissolution of a freeze-dried powder in aqueous solution. Finally, the thermoreversible behavior of these shape-shifting nano-objects was used to construct a first-of-its-kind variable temperature phase diagram to enable the identification of pure spheres, worms, vesicles and lamellae between 6 and 50 °C.
Footnote |
† Electronic supplementary information (ESI) available: Materials and methods; copolymer characterization; SAXS models; GPC data; DSC curves for PHBA homopolymers; FTIR spectra for various (co)polymers; 1H NMR kinetic data; summary table for DLS and TEM data; z-average diameter vs. pH curves and zeta potential vs. pH curves; DLS studies of GA-crosslinked worms; temperature-dependent rheological data; assigned 1H NMR spectra; variable temperature 1H NMR spectra; TEM images for reconstituted spheres, worms, and vesicles; temperature-dependent complex viscosity data, SEM and TEM images of lamellae. See DOI: 10.1039/d1sc05022b |
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