Patrick Florisa,
Damian Connollyb,
Blanaid Whitea and
Aoife Morrin*a
aSchool of Chemical Sciences, National Centre for Sensor Research, Dublin City University, Dublin 9, Ireland. E-mail: aoife.morrin@dcu.ie; Fax: +353 1 700 5503; Tel: +353 1 700 6730
bPharmaceutical and Molecular Biotechnology Research Centre (PMBRC), Department of Chemical and Life Sciences, Waterford Institute of Technology, Waterford, Ireland
First published on 3rd September 2014
Polymer monoliths were prepared in capillary format (250 μm i.d.) and used as solid supports for the immobilisation of the conducting polymer polyaniline (PANI). The immobilisation of PANI was confirmed on the large macro-porous structure of a polystyrene–divinylbenzene (PS-co-DVB) monolith. The surface coverage of polyaniline was characterised by field emission scanning electron microscopy (FE-SEM) and by capacitively coupled contactless conductivity detection (C4D), which was operated in scanning mode to non-invasively visualise the axial distribution of the immobilised PANI and to provide information on its doping state. To further demonstrate the successful functionalisation of the monoliths, the PANI-functionalised monoliths were demonstrated as switchable, weak anion-exchange stationary phases as confirmed by studying the retention of iodide using a perchlorate eluent.
Various electrochemical and chemical syntheses of PANI with a range of resulting morphologies (rods, fibres and spherical particles) have been reported.11 Compared to thick bulk polyaniline films, PANI thin films (<100 nm) results in faster response times and reduced penetration depths for target analytes12 due to the enhanced surface to volume ratio typical of nano materials.
The majority of methods employed for the growth of PANI films on solid substrates are based upon the polymerisation of aniline under acidic conditions using a persulfate oxidant.13 For example Ince et al.14 described the functionalisation of polystyrene (PS) microspheres with PANI for cellulase immobilisation using a two-step approach which involved the electrostatic attachment of aniline on the sulphonated PS surface followed by immersion of the aniline-functionalised spheres in a potassium persulfate solution. This lead to the formation of thick PANI layers (16 μm average depth). Core–shell poly(methyl methacrylate) (PMMA) particles coated with PANI have also been reported.15 A 0.55 μm layer of PANI was formed on the surface of the PMMA cores upon treatment with ethylene glycol dimethacrylate, glycidyl methacrylate and oxydianiline which were used as cross-linking, grafting and swelling agents respectively.
Alternative supports for PANI are monolithic polymer materials which are single, continuous rods of porous polymer. They have been used extensively in chromatography over the last 20 years16,17 because of the high inter-pore connectivity which allows efficient separations to be achieved at high flow rates due to the low pressure-drop across the column. Continuous porous PANI monoliths have been prepared in microfluidic housings as recently described by Gorey et al.18 who demonstrated the fabrication of an inverse-opal conducting PANI monolith via electrochemical growth of PANI within the interstices of a sacrificial PS colloidal crystal template. The monolith's mechanical stability and bonding with the channel walls however, was not fully explored. A more mechanically robust monolith could potentially be prepared by blending PANI with conventional methacrylate- or styrene-based polymers.19 However it is anticipated that this could hinder the electrochemically switchable properties of PANI. For this reason, the immobilisation of a thin film of PANI on an existing monolithic solid support represents a more attractive option in order to counteract this limitation. It also allows the morphology and flow-through properties of the underlying monolith to be easily optimised, independently of a subsequent PANI coating step.
Modifying monoliths with homogeneous thin films of PANI potentially provides an ideal format for studying stimuli-responsive chromatography using conducting polymers. This work builds on that of Wallace in the early 90's where he attempted to study the chromatographic behaviour of these materials on particulate packings.8,20 However the challenge at this time was that in order to create an electrically conducting stationary phase (for use in electrochemically modulated liquid chromatography (EMLC)), particles must be in contact both with each other and with the column walls. This is clearly not the case with particulate stationary phases due to the presence of interstitial voids but could be overcome by moving from a particulate to a continuous support, as described here.
The characterisation of monolithic stationary phases and coatings to date has mainly involved the use of invasive techniques such as FE-SEM or energy-dispersive X-ray spectroscopy (EDX). These techniques are very useful for obtaining visual and qualitative information on the monolith's properties but are only representative of a specific region of the monolith itself and require the sample to be dry. Hence, they do not provide direct information under operational conditions. Recently sC4D has emerged as a useful characterisation tool for monolithic stationary phases,21 especially in capillary format, due to its ability to provide information about stationary phase properties in a completely non-invasive manner. Some recent applications include the evaluation of surfactant coatings on capillary monoliths,22 the verification of structural homogeneity of monolithic rods23 and the visualisation of charged functionalities along monolithic surfaces.24 One distinct aspect of this technique is that the detection is “contactless” since the signal, which is passed through the bore of two ring electrodes placed at a fixed distance apart, is capacitively coupled through the walls of insulating tubing (such as fused silica capillaries).
In the work described here, thermoplastic polymer monoliths were prepared in capillary format (250 μm i.d.) and coated with thin films of PANI. The surface coverage of PANI was visualised by FE-SEM. sC4D was used to non-invasively determine the distribution of PANI along the surface. The switching of PANI from its neutral emeraldine base to charged salt was also indirectly visualised using sC4D. Ion-exchange properties of these stationary phases were also demonstrated, illustrating the potential of these materials as chromatographic stationary phases.
A sC4D profile of the column under acidic conditions was also obtained. The same column was equilibrated for 6 h in 1 mM HNO3 at 3 μL min−1 prior to obtaining readings using the following detector settings: frequency 2× high, input voltage −24 dB and offset 000. A 1 M HCl solution was then flushed overnight at 1 μL min−1 to facilitate protonation of the immobilised PANI. Finally conductivity responses were measured after equilibrating the column in 1 mM HNO3 for 6 h at 3 μL min−1.
It is well known that the nature of both the porogen system and the functional monomer has a significant effect upon monolith pore size26 and so the monolith morphology of each methacrylate monolith was expected to be significantly different from each other. FE-SEM images illustrating the different macro-porous structures of each of the polymer monoliths is given in ESI-4.† Our primary goal however in this work was (a): to investigate the relationship between monolith hydrophobicity and PANI coating integrity and (b): to interrogate the switching properties of the resulting coatings. Therefore, differences in monolith morphology were not considered pertinent in this initial study; in each case the bare unmodified monoliths exhibited suitably low operating back pressures for the flow-through studies.
The formation of PANI aggregates within the pore volume has potential to cause unintentional partial or total blockage of the monolith pores. Thus, FE-SEM imaging was used to evaluate both the integrity of the porous structure before and after PANI polymerisation, as well as the nature of the attachment of PANI to the monolith surface. The AEMA-co-EDMA monolith was intentionally selected as the most hydrophilic monolith in this study and as expected there was no discernable difference in surface roughness after the PANI modification step as shown in Fig. 1(a and b). Conversely, the BuMA-co-EDMA monolith resulted in a fibrillar-like mesh of PANI readily observable on the monolith surface, Fig. 1(c and d). The PANI structures appear not to be intimately bonded to the globule surface but instead appear physically entrapped within crevices between adjacent globules. Operating backpressure (pumping water at 3 μL min−1) increased by 44% after PANI polymerisation, presumably due to partial pore blockage by large PANI aggregates (Fig. 1(d)). Nevertheless, the retention of these PANI aggregates was tentatively attributed to the increased hydrophobicity of BuMA-co-EDMA relative to AEMA-co-EDMA. (It is presumed the weakly bound PANI was rapidly flushed from the AEMA-co-EDMA pore volume during subsequent monolith washing steps). For this reason, a LMA-co-EDMA monolith was employed as a substrate for comparative purposes since it was expected to lead to stronger hydrophobic attachment of PANI films due to its longer alkyl chain (C12) relative to BuMA (C4). Despite the greater hydrophobicity of LMA-co-EDMA monoliths, an unexpectedly patchy surface coverage of PANI was observed after functionalisation, as visualised in Fig. 1(e and f). Here PANI appeared as sparse individual nodules on an otherwise smooth surface. Nevertheless, this was considered a positive development as it was indicative of possible increased dispersive interactions between PANI and the C12 alkyl chain of LMA (along with dipole–dipole interactions given that the monolith was methacrylate based). Flow-through properties were not adversely affected for the PANI-coated LMA-co-EDMA monolith (with backpressures of 0.9 bar per cm at 3 μL min−1).
In order to examine the effect of other interactions such as potential π–π interactions between the underlying monolith and PANI thin films, a PS-co-DVB monolith was prepared, again using a monomer/porogen composition which ensured a comparatively low operating backpressure.26 Previous reports which describe the preparation of PANI-modified PS spheres involved an initial sulphonation of the PS in order to achieve a negatively charged surface which facilitated electrostatic binding of protonated aniline molecules prior to their polymerisation. Interestingly, prior sulphonation of the PS-co-DVB monolith was found to be unnecessary in this work, with the PANI formation step performed as per the methacrylate monoliths, thereby allowing a direct comparison of PANI coverage to be made.
Post-functionalisation of the PS-co-DVB monolith, a green colour along the entire monolith length was visible through the fused silica capillary housing. This was indicative of the emeraldine salt form of PANI and could readily be reversibly switched to a homogeneous violet colour (the emeraldine base form of PANI) by flushing the monolith overnight with 1 M NaOH as shown in Fig. ESI-2.† A marked improvement in PANI coverage over the methacrylate-based polymer monolith supports was observed (Fig. 1(g and h)) in which a PANI film with a nano-structured morphology evenly coats the PS-co-DVB monolith globules.
The modification process on the PS-co-DVB monolith was repeated up to 3 times which, as illustrated from the FE-SEM images shown in Fig. ESI-5,† lead to an apparent increase in the thickness of the PANI coating which appeared as an interconnected network with bud-like features. A small increase in operating backpressure from 0.2 to 0.3 bar per cm at a nominal flow of 3 μL min−1 was observed after modification with three coatings of PANI suggesting no dramatic change in flow-through properties of the monolith occurred. Further studies are required to determine the PANI coating thickness. The affinity of PANI for the monolith surface was attributed to both hydrophobic and π–π interactions between the benzene rings present in both aniline and the monolith backbone.27,28 In this study, PS-co-DVB monoliths clearly represented the most ideal monolithic support for PANI adsorption given the coating homogeneity observed by FE-SEM.
For a PANI-modified monolith to be useful for stimuli-responsive chromatography, the axial homogeneity of the PANI coating is critical; any gaps or fissures in the coating could impede its switching, e.g., if the stimulus was electrical in nature and as such relied on a continuous film. Recently, reports illustrating the benefits of sC4D for non-invasively characterising monolithic stationary phases in capillary formats have appeared in the literature. For this reason sC4D was utilised in an effort to confirm the presence of PANI on the surface of the monoliths and potentially visualise pH switching of the chemical PANI state by way of this conductive response.
The conducting properties of PANI depend on its oxidation state and on the presence and nature of a dopant anion. Electron mobility is facilitated by the presence of a conjugated double bond structure which results in electron delocalization and facilitates the control of its conductive and insulating properties. It is known that under acidic conditions PANI is in a “doped” conductive state (the emeraldine salt form) with conductivity values that range from 10−2 to 100 S cm−1. When exposed to strong bases however, PANI is reversibly converted to an insulating state (the emeraldine base form) and its conductivity decreases to values ranging from 10−10 to 10−7 S cm−1.31
As illustrated in Fig. 2, the monoliths were subjected to sC4D characterisation before and immediately after modification with PANI using a constant flow of 1 mM HNO3 in order to dope the PANI coating. The scales of the detector responses in each graph has been normalised in order to allow a comparison between conductive responses for each monolith upon modification with PANI. Profiles of monoliths AEMA, BuMA and LMA illustrated in Fig. 2(a–c) respectively, showed negligible changes in conductive response after modification with PANI (e.g. a maximum change of +60 mV for the AEMA monolith was observed). This is clearly visible from the zoomed-in conductive profiles of monoliths AEMA, BuMA and LMA shown as insets in Fig. 2(a–c) respectively. Conversely, a larger increase in conductive response (relative to the neutral uncoated monolith) was observed for the PS-co-DVB monolith in Fig. 2(d). The blank PS-co-DVB monolith displayed a homogeneous conductive response shown in Fig. 2(d)(i), indicating that no major defects in the monolith structure (e.g. localised areas of incomplete polymerisation) were present. Upon modification with PANI, shown in Fig. 2(d)(ii), sC4D measurements revealed a 45% increase in conductive response. After a single modification, the presence of a non-homogeneous film was evident (most prominent in the initial 25–45 mm of column). After a second and third modification, shown in Fig. 2(d)(iii) and (iv) respectively, improved homogeneity in coverage was observed. The steep rise in conductivity observed after modification in the region between 65–75 mm of the column may be attributed to a localised pre-concentration effect during the functionalisation steps. This is visualised on one end of the column only since the initial 2 cm at the other end were covered by a connecting sleeve and hence remained uncharacterised. Two additional PS-co-DVB monoliths were subjected to the 3-step PANI coating process with sC4D profiling also performed at each intermediate stage. The profiles in Fig. ESI-6† show that the PANI-coating procedure was repeatable on each monolith, with an increasing conductive response observed for each subsequent PANI coating, suggesting that the coating integrity improved after each PANI polymerisation step. Interestingly, sC4D could be used in all cases to verify the presence of an inhomogeneity of coverage at the extremities of each monolith (which could easily be removed by cutting, before using the monoliths for subsequent chromatographic applications).
The inset in Fig. 3(a) represents a zoomed-in view of the conductive profiles of the monolith before and after modification. Measurements were performed in triplicate and low standard deviation values were obtained (±5 mV) indicating the reproducibility of the measurement. In a further step, the same column was characterised in 1 mM HNO3, shown in Fig. 3(b)(i). It can be seen that under these conditions, full protonation of the immobilised PANI was not achieved. To enable complete protonation, 1 M HCl was flushed through the column to allow the switching of PANI into the emeraldine salt conductive form (observed as a green colour along the monolith length). This was confirmed again by obtaining sC4D readings in 1 mM HNO3, shown in Fig. 3(b)(ii), where a 70% increase in conductive response relative to the same column prior to protonation was observed. For comparative purposes, the sC4D profile of an unmodified PS-co-DVB monolith, (Fig. 3(b)(iii)), was also included which had a similar profile to that obtained for the PANI-functionalised monolith in the dedoped (non-conducting) state.
Retention of iodide was also observed on the same column. Due to the low ion-exchange capacity of the stationary phase, a low ionic strength eluent which could also be an appropriate supporting electrolyte (0.1 mM perchlorate) was used.32 Upon injection of a water blank, shown in Fig. 4(c), a void peak was visualised just before 5 min. After the injection of 1 mM iodide, shown in Fig. 4(a), a positive peak was visualised at 9.7 min which was indicative of the ion-exchange properties of the PANI-modified monolith. By flushing a 1 M solution of NaOH through the column in a further step, it was possible to de-dope the immobilised PANI. The absence of a peak at 9.7 min after the injection of iodide, shown in Fig. 4(b) confirmed that the PANI-coated monolith in the de-doped state no longer behaved as an ion-exchanger. The small ion-exchange capacity observed demonstrated that the emeraldine salt form of PANI was present on the surface of the PS-co-DVB monolith and could exchange its chloride dopant with ions in solution. The value calculated however is low in comparison to previously reported ion-exchange monolithic stationary phases.33 A possible explanation of this can be related to the deprotonation of imine nitrogens which occurred by flushing a non-acidic eluent such as perchlorate. Furthermore, the large macro-porous structure of the monoliths used here resulted in a very low surface area which would translate into limited chromatographic efficiency. Nonetheless the ion-exchange capacity of these materials has been demonstrated in principle.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra05565a |
| This journal is © The Royal Society of Chemistry 2014 |