Yan
Kang
,
Anaïs
Pitto-Barry
,
Anna
Maitland
and
Rachel K.
O'Reilly
*
Department of Chemistry, University of Warwick, Gibbet Hill Road, Coventry, CV4 7AL, UK. E-mail: Rachel.oreilly@warwick.ac.uk
First published on 11th June 2015
The synthesis and self-assembly of thymine-containing polymers were performed using RAFT dispersion polymerization. A combination of microscopy and scattering techniques was used to analyze the resultant complex morphologies. The primary observation from this study is that the obtained aggregates induced during the polymerization were well-defined despite the constituent copolymers possessing broad dispersities. Moreover, a variety of parameters, including the choice of polymerization solvent, the degree of polymerization of both blocks and the presence of an adenine-containing mediator, were observed to affect the resultant size and shape of the assembly.
Recently we have demonstrated the synthesis of nucleobase-containing materials using RAFT dispersion polymerization.28 In our previous study, poly(methyl methacrylate) (PMMA) was used as the macro-CTA and only adenine-containing monomers or a mixture of adenine-containing monomers and thymine-containing monomers were used to chain extend the PMMA block. RAFT dispersion polymerizations were investigated in both chloroform and 1,4-dioxane. It was found that using these conditions polymers obtained were generally well-controlled in terms of molecular weight and molecular weight distribution. Moreover, it was also observed that the choice of polymerization solvent played a key role in the final morphologies achieved.
Thymine is one of the natural nucleobases in DNA and binds to adenine via complementary hydrogen bonding interactions to stabilize DNA and enable the formation of a double helix. Moreover, it is also well-known that thymine can form triple hydrogen bonds with diaminopyridine or its derivatives.23,24 Based on these properties, thymine is commonly used for controlling polymer tacticity,29 templating polymerizations,30–32 facilitating molecular self-assembly and aggregation33–36 and protecting active moieties.37 However, there are still few reports on the systematic study of the self-assembly of thymine-containing polymers of various lengths.33,38 Considering the advantages of RAFT dispersion polymerizations, we have applied this approach to readily prepare a variety of thymine-containing nanostructures. However, compared to our previous work on RAFT dispersion polymerization to prepare nucleobase-containing nanostructures,28 contrasting results in terms of morphology and molecular weight distributions of the resultant polymers have been observed. Indeed, in the pure thymine system the produced morphologies are more varied and better defined despite the fact that the resultant polymers are bimodal in most cases. This contradicts current thinking that narrow dispersity block copolymers are a prerequisite for the formation of well-defined assemblies.39 However, this study shows that well-defined nanoobjects can still be attained although the constituent block copolymers possess broad dispersities (ĐM often greater than 1.5). Indeed, the study of the solution behavior of polydisperse block amphiphiles is of growing scientific interest.40–48 It is known that block copolymers with broad dispersities affect the interfacial curvature, which allows structures with non-constant interfacial mean curvatures, but that are thermodynamically stabilized, to form (e.g., prolate-spheroid micelles,40 stabilized vesicles,43 and more complex structures42,49). In order to further extend this concept we have performed RAFT dispersion polymerizations of a thymine-containing monomer, which under varying conditions can undergo hydrogen-bonding to allow for more complex polymerization procedures. To explore this fully a range of polymerization conditions were explored and their effect on the resultant morphologies and polymers investigated. Such functional polymers, capable of intra- and inter-molecular H-bonding interactions are an interesting emerging class of new materials which enable access to novel morphologies and can provide an insight into the self-assembly process of such complex functional polymers.
Size exclusion chromatography (SEC) was performed in HPLC grade DMF containing 5 mM NH4BF4 at 50 °C, with a flow rate of 1.0 mL per minute, on a set of two PLgel 5 μm Mixed-D columns, plus one guard column. SEC data was analyzed with Cirrus GPC software calibrated using polymethyl methacrylate (PMMA) standards. The SEC was equipped with both refractive index (RI) and UV detectors.
Transmission electron microscopy (TEM) was performed on a JEOL 2000FX electron microscope at an acceleration voltage of 200 kV. All TEM samples were prepared on graphene oxide (GO)-coated carbon grids (Quantifoil R2/2) which allows high contrast images to be acquired without staining.53 Generally, a drop of sample (20 μL) was deposited on a grid which was placed on a piece of filter paper and then left to air dry.
Hydrodynamic diameters (Dh) and size distributions of the self-assemblies were determined by dynamic light scattering (DLS). The DLS instrumentation consisted of a Malvern Zetasizer NanoS instrument operating at 25 °C with a 4 mW He–Ne 633 nm laser module. Measurements were made at a detection angle of 173° (back scattering), and Malvern DTS 6.20 software was used to analyze the data. The viscosity of the mixtures of CHCl3 and 1,4-dioxane is estimated by a simplified equation.54
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Static light scattering (SLS) measurements were performed using an ALV CGS3 (λ = 632 nm) at 20 °C. The data was collected from 12° up to 30° with an interval of 2° or 30° up to 150° with an interval of 10° and calibrated with filtered toluene and filtered CHCl3 as backgrounds. The refractive index increment of the polymer in CHCl3 was measured to be 0.053 mL g−1.
Small-angle neutron scattering (SANS) experiments were recorded at the ISIS neutron beam facility, on the sans2d instrument at the Rutherford Appleton Laboratory, Oxford. Samples were measured at 20 mg mL−1 in CDCl3, which provides high contrast in scattering length for the polymer. Small-angle X-ray scattering (SAXS) experiments were carried out on the SAXS-WAXS beamline at the Australian Synchrotron facility at a photon energy of 15 keV. The samples were prepared in 1,4-dioxane and were run using 1.5 mm diameter quartz capillaries. The measurements were collected at 25 °C with a sample to detector distance of 7.160 m to give a q range of 0.0015 to 0.08 Å−1, where q is the scattering vector and is related to the scattering angle (2θ) and the photon wavelength (λ) by the following equation:
All patterns were normalized to fixed transmitted flux using a quantitative beam stop detector. The scattering from the solvent was measured in the same location as sample collection and was subtracted for each measurement. The two-dimensional SAXS images were converted into one-dimensional SAXS profiles (I(q) versus q) by circular averaging, where I(q) is the scattering intensity. ScatterBrain and NCNR Data Analysis IGOR Pro software were used to plot and analyze SAXS and SANS data.55 The scattering length density of the solvents and monomers were calculated using the “Scattering Length Density Calculator” provided by the NIST Center for Neutron Research.56
The synthetic route for the PMMA macro-CTA synthesis (2 and 3) is shown in Scheme 1. CPDT was used as the CTA as it is suitable for the polymerization of methacrylates and the polymerizations were stopped at relatively low conversion <60% to ensure good end group fidelity. The DP of the PMMA macro-CTA was determined by 1H NMR spectroscopy by comparing the integration of PMMA backbone signals with those of the CPDT end group. The resulting DPs of PMMA were ca. 70 (polymer 2) and 220 (polymer 3). SEC (DMF as eluent, PMMA standards) was used to further determine the molecular weight and the molecular weight distribution. In addition to the observed narrow molecular weight distributions, the molecular weights from SEC are consistent with the results from 1H NMR spectroscopy. Furthermore, the RI SEC trace and UV SEC trace (λ = 309 nm from trithiocarbonate end group) overlap well, suggesting good end group fidelity (Fig. S2†).
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Scheme 1 Synthetic route for the macro-CTAs (PMMA, 2 and 3) and the thymine-containing diblock copolymers using RAFT dispersion polymerization (4–9). |
RAFT dispersion polymerizations of TMA were performed at 60 °C using 2 or 3 as the macro-CTA and AIBN as the initiator. The conversions of the polymerizations were determined by 1H NMR spectroscopy and the molecular weight and molecular weight distributions were analysed by SEC (DMF as eluent, PMMA as standards). The morphologies induced during the polymerizations were characterized by both light scattering and microscopy analysis. To explore the polymerization parameters more fully and understand the dispersion polymerization procedure a range of conditions (including solvent quality, nucleobase block length, addition of a mediator) were utilized to prepare the block copolymers and nanostructures.
Under these different solvent conditions a range of assembly morphologies were obtained for the targeted block copolymer PMMA70-b-PTMA100. When pure chloroform was used as the polymerization solvent, a bimodal molecular weight distribution was observed by SEC and only well-defined aggregates (ca. 200 nm) were observed by light scattering (Table S1 4–100 and Fig. S3†). Examination of the reaction mixture by dry state TEM indicated that vesicles were formed during the dispersion polymerization (Fig. 1a, 4–100). To eliminate the possibility of imaging artefacts caused by imaging particles in the dry-state, SLS was also conducted on the sample to further determine the morphology (Fig. S3†). A Zimm analysis revealed that the P-ratio (Rg/Rh, ratio between radius of gyration and hydrodynamic radius) of the nanostructures was close to 1 (Rg/Rh = 1.17), indicating the formation of hollow structures.57,58 SANS was also conducted on a more concentrated sample (20 mg mL−1), which was obtained directly from the polymerization solution without dilution (Fig. S4†). The Guinier-Porod fit was firstly applied to confirm a spherical shape for these assemblies.59 Furthermore, the thickness of the vesicle membrane was determined from a plot of q2I(q) versus q.60 The first minimum of this plot q corresponds to the first zero of the membrane factor given by:
d = 2π/q |
When a mixture of chloroform and 1,4-dioxane (volume composition of chloroform: 75%) was used as the solvent (Table S1 4–75, Fig. S5†), once again a bimodal polymer formed and a more complex morphology was observed. In this case lamellae with tentacles were observed by TEM analysis (Fig. 1b, 4–75). These assemblies appeared well defined by DLS analysis and had a hydrodynamic diameter of ca. 300 nm. AFM analysis was conducted on this sample, which further confirmed the formation of lamellae with tentacles morphology. Moreover, it showed the height of the lamellae and tentacles were ca. 25 and 35 nm, respectively (Fig. S6†). Further decreasing the volume composition of chloroform during the polymerization to 50% led to the formation of long flexible cylinders (Table S1 4–50, Fig. S7†). From TEM analysis, the cylinders were around 5 μm long (Fig. 1c, 4–50). Even longer and thinner cylinders were observed when the compositions of chloroform were 33% and 25%, respectively (Fig. 1d, 4–33 and 1e, 4–25; Fig. S8 and S9†). These cylinders were more than 10 μm in length and around 55 nm in width by TEM analysis. However, when the amount of chloroform used in the dispersion polymerization was dropped to 12.5%, much shorter worm-like structures were obtained (Fig. 1f, 4–12.5; Fig. S10†) and the width of cylinders slightly increased to 75 nm. DLS was also used to analyze the resultant morphologies. However, due to the highly elongated structures obtained in these systems, the sizes obtained from DLS are relative values.62
In the case of pure 1,4-dioxane as the polymerization solvent, low contrast disk-like structures with a diameter of ca. 100 nm were observed by TEM analysis (Fig. 1g, 4–0; Fig. S11†). AFM was then conducted on this sample and the heights of the structures were ca. 3–5 nm (Fig. S12†), which confirmed the disc-like morphology. SAXS was used to further analyze the morphology in solution (Fig. S13†). Kratky plots for spheres and cylinders were plotted with the raw data to emphasize the deviation of the scattering intensity at high-q values. The sphere plot (q2I(q) versus q) showed a horizontal asymptote at high q values which suggests the presence of spheres. In the meantime the cylinder plot (qI(q) versus q) also tended to a horizontal asymptote at high-q values thus confirming the presence of cylinders in solution. Such plots can suggest the assemblies have both spherical and cylindrical features. Slopes of −1 and −2 were observed in the log(I(q)) versus log(q) plot, which suggests the presence of rods with a very short length. Finally different models were applied and attempts to analyze this profile with a disperse spherical uniform model,61 uniform convex lens,63,64 or uniform cylindrical models (with short length to account for a disk-like morphology)59 yielded poor quality data fits. This suggests that the morphologies were not convex lenses, simple spheres or disks. Indeed, a core–shell cylindrical model with dispersity in the core radius provided the best results (Fig. S13†).59 This fit suggested that structures were formed with a core radius of ca. 9 nm, a corona thickness of ca. 8 nm and a core length or depth of ca. 3 nm, suggesting the formation of disk-like structures. Whilst this fit was the best of those examined, the quality was not as good as expected. Moreover, the large difference of dimensions obtained between the structure models utilized in the SAXS analysis and the TEM analysis suggests that the former did not reflect the entire sample. This may be due to a solvation effect or large sample dispersity in either diameter or height. Given the observations made by TEM analysis it is suggested that the dispersity is in the height of the disk rather than the diameter.
Overall, these results show that various morphologies can be accessed by varying the composition of solvent during the RAFT dispersion polymerization of TMA. However, the polymers obtained under the range of polymerization solvents were not monodisperse (Fig. S14†). Indeed bimodal chromatograms were observed by SEC analysis in each case. To eliminate the possibility that TMA monomer had undergone side-reactions during the polymerization, mixtures of TMA and CPDT were stirred at 60 °C in chloroform under N2 atmosphere for 24 hours. Monitoring by 1H NMR spectroscopy analysis, there was no obvious change observed before and after heating, which indicated that both TMA and the chain transfer agent were stable under the polymerization conditions (Fig. S15†). Therefore, it was concluded that the observed bimodal distributions of the polymers were induced by the RAFT dispersion polymerization process.
Thus, with decreasing TMA block length and hence increasing weight fraction of PMMA from 54 to 32 to 19%, as expected a morphology transition, from sphere to cylinder to vesicle was observed in the dispersion polymerization performed in chloroform. This observation is consistent with the previous observation in the literature for RAFT dispersion polymerizations, however it is interesting as the polymers in this work have much broader polydispersities which does not seem to affect the self-assembly process.13
In comparison, when 1,4-dioxane was used as the polymerization solvent, a sphere-cylinder-vesicle transition was not observed when increasing the block length of TMA from 50 to 200 (Table S1, 6b, 4–0, 7, 8; Fig. S19–S24†). Instead across the PMMA composition range (from 32 to 19 to 14 to 11 weight%, for polymers 6b, 4–0, 7, and 8, respectively) only larger micelles were observed which increased in size (from 21 to 341 nm) as the DP of the PTMA block increased. The possible reason for this observation is that the nucleobase polymers have better solubility and weaker intra- and intermolecular chain interactions in 1,4-dioxane than chloroform (Ka = 12 versus 20 M−1 at 60 °C). It has been shown by van Hest, for related nucleobase systems, that solvents such as water lead to a higher than calculated lypophilic fraction, which in turns leads to the formation of spherical micelles across a broader composition window.38
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Scheme 2 Synthetic route for the thymine-containing diblock copolymers using RAFT dispersion polymerization in the presence of adenine-mediator. |
RAFT dispersion polymerization was carried out in the presence of the adenine-containing mediator (amount of TMA:
mediator = 1
:
1) using PMMA70 as the macro-CTA and chloroform as the solvent. The studied DPs of the thymine-containing block were 20, 50, and 100 (Scheme 2, to afford polymers 5′, 6a′, and 4–100′ respectively). When the DP of the thymine-containing block was 20, small spherical micelles were obtained (Fig. 3a, 5′), which was very close to the morphology obtained in the absence of the mediator (Fig. 2a, 5). Moreover, the dispersity of the resultant copolymer obtained in the presence of the mediator was much narrower compared to the copolymer obtained in the absence of mediator (Fig. 3d and S26†). However, the monomer conversion was also lower (66%) perhaps due to the improved solubility of TMA in the presence of mediator, which changes the kinetics from a dispersion polymerization to a solution polymerization.
In the case of the DP 50 TMA block, spherical micelles were observed in the presence of the mediator (Fig. 3b, 6a′), which is different from the polymerization performed, under identical conditions, without the addition of the mediator (Fig. 2b, 6a where cylinders were formed). In the presence of the adenine-containing mediator, the solubility of PTMA in chloroform increases, which decreases the apparent packing parameter of the assembly,67 therefore spherical micelles were formed instead of cylinders.
Further increasing the DP to 100 resulted in the formation of vesicles (Fig. 3c, 4–100′; Fig. S28†) similar to that observed for the polymerization without mediator (Fig. 1a, 4–100). However, in this case the vesicles possessed wrinkled membranes, which are thought to be due to the complementary interactions between the PTMA and adenine-containing mediator disrupting the assembly process. Overall, addition of an adenine-containing mediator does not significantly change the observed morphology for the series of PTMA block copolymers. Moreover, a narrowing of the dispersity of the resultant copolymer is only observed for the short thymine-containing block and for the longer thymine-containing blocks, little effect on dispersity is observed.
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Fig. 4 Representative TEM images of self-assemblies prepared by RAFT dispersion polymerization for a target copolymer PMMA220-b-PTMA50 in (a) 9a, chloroform; (b) 9b, 1,4-dioxane. Scale bar: 100 nm. |
In contrast, when 1,4-dioxane was used as the solvent the resultant self-assembly, 9b, was not well-defined as determined by both TEM and DLS analysis (Fig. 4b and S30†). From TEM analysis, a phase-separated pattern was observed and by DLS a broad and fluctuating distribution suggested that the resultant structures were not stable in solution. In this case it was observed that the resultant polymer, 9b, has a significantly narrower dispersity than the related polymers prepared in chloroform (9a) or with the shorter macro-CTA (4–0) due to the improved solubility of the growing diblock in 1,4-dioxane (Fig. S30†).
In this study, nearly all the block copolymers obtained were bimodal by SEC analysis, despite this the resultant self-assemblies were surprisingly well-defined and predictable. In a dispersion polymerization, polymerization proceeds in the polymer particles as they absorb monomers from the continuous phase,68 however, in our system as the pyrimidine–pyrimidine interactions are relatively weak (compared to purine–purine interactions) and the monomer has good solubility in the polymerization solvent, we hypothesize that the monomer absorption into the core of the particles is modest and thus the aggregates can readily establish a thermodynamic equilibrium, which leads to the formation of well-defined structures despite the broad dispersity of the constituent copolymers.
Footnote |
† Electronic supplementary information (ESI) available: 1H NMR spectra, SEC, DLS, SANS, SAXS, SLS data. See DOI: 10.1039/c5py00617a |
This journal is © The Royal Society of Chemistry 2015 |