Maria Grzeszczuk* and
Rabia Ozsakarya†
Faculty of Chemistry, University of Wrocław, 14 F. Joliot-Curie, 50-383 Wrocław, Poland. E-mail: maria.grzeszczuk@chem.uni.wroc.pl; Tel: +48 71 3757336
First published on 8th May 2014
Polypyrrole layers were deposited on polycrystalline gold from solutions of pyrrole in the ionic liquid 1-butyl-3-methylimidazolium tetrafluoroborate and its equimolar mixture with water by using potential controlled electrochemical methods. Cyclic voltammetry, electrochemical impedance spectroscopy, scanning electron microscopy and dispersive X-ray microanalysis were characterization methods of polymeric products. The morphology of the solution side of the polymer layers depended on the composition of the polymerization bath and layer thickness. Correlations between impedance parameters and surface morphologies were investigated. Intermolecular interactions in the ionic liquid and in its mixture with water were invoked to discus packing motifs of the polypyrrole chains deposited on gold. Different morphologies of the polypyrrole films, from a crystal-like solid to a colloid semi-rigid liquid, were observed for the submicrometer films. Values of the double layer impedance frequency dispersion parameter as well as elemental microanalysis data are consistent with the surface morphology images. The charge transport processes of the polypyrrole electrode are impacted by the morphology as well as thickness of the thin polymer films. The ionic liquid electrolytes can be used to tailor the micro and nanostructures of electrodeposited polypyrrole.
The research activity in the field of ionic liquids or room temperature ionic liquids (ILs or RTILs) has increased dramatically during the last years. Also their use as an environmentally friendly alternative for conventional solvents has gained much attention in electrochemical research and applications.5 Room temperature ionic liquids have been presented in chemistry as a new class of solvents for extraction processes and organic reactions, both for catalyzed and uncatalyzed.6 The organic molten electrolytes, especially those at or near ambient temperature, have been the focus of many scientific investigations since a long time because of their specific physical and chemical properties.7 Ionic liquid solvents with non-flammability and non-volatility can dissolve a wide range of organic and inorganic compounds. For usefulness in electrochemistry high ionic conductivity, good thermal stability and a wide electrochemical window should characterize them.8
In recent years, ILs have been used in polymer science, mainly as polymerization media in several types of polymerization processes, including conventional free radical polymerization.9 Furthermore, as electrolytes with wide potential windows and high ionic conductivity, the air and moisture stable ILs are expected to be peculiarly suitable medium for electropolymerization and applications in π-conjugated polymer electrochemical devices.10
The properties of ionic liquids can be adjusted by choosing specific combinations of cations and anions. For instance, they can be made either hygroscopic or hydrophobic. The number of already described and potential cation–anion combinations is very large. Typically ionic liquids are composed of bulky 1,3-dialkylimidazolium, alkylammonium, alkylphosphonium or alkylpyridinium organic cations and inorganic anions such as most frequently AlCl4−, BF4− or PF6− but also NO3−, ClO4−, CF3COO−, CF3SO3− or CH3COO− and other anions. The most commonly known ionic liquids include 1-butyl-3-methylimidazolium hexafluorophosphate and tetrafluoroborate abbreviated as BMIMPF6 and BMIMBF4, correspondingly. However the two salts differ substantially regarding miscibility with water. In this study, water miscible BMIMBF4 was used. Electropolymerization of pyrrole and subsequent characterization of the resulting polymer in BMIMBF4 environment were not yet reported to the best of our knowledge. A general advantage of using the ionic liquid solvents over other electrolytes for electropolymerization and subsequent electrochemical processing might result from their wide potential and temperature windows.
A main purpose of this study was to carry out electrooxidative polymerization of pyrrole in the ionic liquid using the potentiostatic and cyclic potentiodynamic electrolytic regimes and investigate influence of the electrolyte on properties of the polymer electrode using cyclic voltammetric (CV) and impedimetric (EIS) characterization of the electrodeposited polypyrrole (PPy). Scanning electron microscopy (SEM) images of the resulting polymer electrodes were taken to reveal their surface morphology and energy dispersive X-ray (EDX) elemental microanalysis was used as well. Furthermore, an influence of water added to the electropolymerization medium on the electrochemical performance of the polymer was followed. So far, no reports have appeared on redox and impedance characteristics of a conducting polymer electrodeposited in presence of and without water in a liquid salt. Consequences of polypyrrole deposition in BMIMBF4 (freshly dried or after storage) and in equimolar BMIMBF4–H2O solution on electrochemical characteristics (CV, EIS) of the polymer films in BMIMBF4 as well as on their corresponding surface morphology (SEM) and composition (EDX) are shown.
Four gold electrodes (Au1, Au2, Au3, Au4) were used in two polymerization sessions. Before polymerization, the potential window of Au in the ionic liquid was checked in. After the potential window was determined, 0.07 ml pyrrole was put into 10 ml volume of the ionic liquid to give 0.1 M monomer solution concentration, which corresponds to 0.02 molar quotient of pyrrole in BMIMBF4.
In a first synthesis session, Au2 and Au3 were used to produce polypyrrole with the potentiodynamic method, Au4 was used with the potentiostatic method and Au1 was used with a combination of the both methods. Then the samples were designated as Au2/PPy, Au3/PPY, Au4/PPy and Au1/PPy, respectively. Au4/PPy was obtained in a multistage procedure, which started and ended with potentiostatic depositions at 1.0 V and 1.2 V respectively. Au1/PPy was obtained under successive potentiostatic at +0.9 V for 1000 s and (−0.65, +1.1) V at 0.05 V s−1 CV regimes, 80 scans: Au3/PPy was prepared under (−0.55, +1.1) V CV at 0.1 V s−1, 100 scans: Au2/PPy was prepared under (−0.65, +1.1) V CV at 0.1 V s−1, about 100 scans.
In a second synthesis session, only three substrate gold electrodes were used: Au2 and Au3 for the potentiodynamic syntheses in potential range (−0.6 V, +1.1 V), and Au4 for the step by step potentiodynamic syntheses in the potential ranges from −0.6 V to +0.8 V, +0.9 V and +1.0 V in the three successive steps, respectively. Then the later samples were designated as Au2a/PPy, Au3a/PPy and Au4a/PPy, respectively. Note that the legends of the figures and tables contain description of the synthesis relevant to the data reported there. Amount of electric charge consumed for the polymer deposition differed from sample to sample but was not larger than 0.3 C cm−2 (8.9 mC/0.03 cm2) and thus corresponded to thickness of the order of 10−1 μm for the most PPy films, except for Au4/PPy where it was of the order of 1 × 100 μm.11,12
After each polymerization the electrodes were washed with acetonitrile to remove the ionic liquid remaining into the polymer films and then dried at room temperature in a desiccator.
Later on, ex situ SEM images of the polypyrrole electrodes were made using HITACHI S-3400 N scanning electron microscope. The X-ray (EDX) microanalysis method for quantitative characterization of the polymer films was inspected as well.
Fig. 2 Progress of polypyrrole deposition on Au2 by the cyclic potentiodynamic method in 0.1 M pyrrole–5.3 M BMIMBF4. |
The products of the two fore mentioned polymerization procedures were characterized by CV and EIS.11 Voltammograms of the three independent polymer samples are shown in Fig. 3. The redox activity measured as a mean anodic/cathodic charge involved in the redox switching, when assumed to correlate with a yield and thickness of polypyrrole, indicate the following order of polymer layer thickness: Au1/PPy > Au3/PPy > Au2/PPy.
Electrochemical impedance spectra of the polypyrrole films being under comparison were collected in the same frequency regions containing the same number of frequency data points, at electrode potentials corresponding to different reversible oxidation levels of the polymer. The (100 kHz, 5 mHz) spectra for the PPy samples oxidized at +0.2 V are compared in Fig. 4. Changes in the impedance magnitude follow that evidenced by the cyclic voltammograms thus resulting mainly from differences in the polymer layer thickness. In general, the imaginary component of the impedance decreases with thickness as a consequence of an increased capacitance of the film. The lowest frequency Z′′ values bear a dominant contribution from the redox pseudocapacitance of polypyrrole. Thus so, a higher capacitance (a lower Z′′) is observed for a thicker film. The higher frequency ranges of the spectra, shown in the bottom of Fig. 4, point out more resistive impedance of the Au3/PPy as compared with thicker (Au1/PPy) and thinner (Au2/PPy) films. Remarkably, no parts of the spectra in this range resembles the pure Warburg impedance behavior, which means fast ionic diffusion and/or special diffusion paths similar to that observed for a crystalline oxide material.12
The EIS data can be analyzed on a quantitative basis using the equivalent electrical circuit approach. The ladder type circuit structure was assumed for the polypyrrole electrode and, using the Boukamp's circuit code, the experimental data were fitted to the R0(Q1[R1(Q2T)]) circuit shown also in Scheme 1.15
There, R0 is the electrolyte resistance (ionic liquid), R1 is the charge transfer resistance of the polymer electrode (ionic liquid/polypyrrole film interface), Q1 and Q2 are the constant phase elements – the general diffusion related frequency dispersions corresponding to fast (double layer) and slower (adsorption) processes of the polymer electrode, respectively. T is the finite length diffusion element characteristic for diffusion through a medium where one boundary is blocking for the diffusing species (Au surface blocks ions diffusing through the polymer). The frequency dispersion admittance functions of elements Q and T are as follows, respectively:15
YQ = Y0,Q(jω)n with 0 < n< 1 | (1) |
(2) |
The parameters of the best CNLS (complex nonlinear least squares) fits of the experiment – simulation data are collected in Table 1.
Parameter/electrode | Au2/PPy | Au3/PPy | Au1/PPy |
---|---|---|---|
R0/kΩ | 0.64 | 1.30 | 0.77 |
2% | 1% | 1% | |
R1/kΩ | 3.67 | 33.4 | 2.21 |
4% | 2% | 4% | |
Y0(Q1)/Ω−1 s+n | 1.6 × 10−6 | 0.9 × 10−6 | 3.5 × 10−6 |
12% | 3% | 10% | |
n(Q1) | 0.65 | 0.61 | 0.63 |
2% | 1% | 2% | |
Y0(Q2)/Ω−1 s+n | 4.7 × 10−6 | 4.9 × 10−6 | 7.3 × 10−6 |
6% | 1% | 7% | |
n(Q2) | 0.77 | 0.60 | 0.74 |
1% | <1% | 2% | |
Y0(T)/Ω−1 s+1/2 | 1.3.0 × 10−6 | 0.7 × 10−6 | 5.7 × 10−6 |
10% | 9% | 3% | |
B(T)/s1/2 | 1.0 | 3.4 | 1.9 |
5% | 5% | 1% |
One should note that the most impedance parameters for the thinnest of these films (Au2/PPy) are similar to those of the much thicker film prepared by the sequential method (Au1/PPy). The impedance characteristics of the three films seem to originate from their thickness and surface morphology. The possibly lowest effective surface area of the Au3/PPy film may be related to the biggest size of the polymer particulates at the surface of the electrolyte (compare Fig. 5 and 6). So, the smaller particles enhance the interfacial ion transfer and impact the bulk film conductance processes by lengthening the ionic diffusion paths.
Fig. 5 SEM micrographs of the polypyrrole films Au2/PPy (top) and Au3/PPy (bottom), deposited in BMIMBF4 using the cyclic potentiodynamic method. |
Fig. 6 SEM micrographs of the polypyrrole film Au1/PPy deposited in BMIMBF4 using the initial potentiostatic and final cyclic potentiodynamic deposition steps. |
The structure of ionic liquids is known to differ substantially from the structure of conventional molecular liquids. The liquid salts reveal a higher degree of molecular ordering and are sometimes called the nano-structured fluids as they can keep locally a molecular ordering resembling the crystal structure of the solid state salt.20 The resulting local liquid crystal structure motifs may be copied on the polymer chain arrangement as the later is determined by the anion doping of the oxidized polymer precursor species formed during the electrooxidative process of pyrrole. The results of single crystal X-ray analysis of the BMIM+ salts show that the cations and the halogen anions form characteristic column structures.20 The butyl group rotational isomers of BMIM+ influences the cation subsystem structures and then the anion subsystem adjust as well. It is likely that the zigzag anion chains found in the crystals of BMINCl exist in the liquid state of the BMIN+ salts as well. The polypyrrole particles with a geometry of their edges resembling rather crystals than usual round edged cauliflower morphologies may follow from the dominant arrangement pattern of counter-anions in liquid BMIMBF4 at a polymer deposition front.
In addition, SEM micrographs of our polypyrrole layers point out significant influence of thickness and/or the synthesis method on morphology of the surface. A SEM image of Au1/PPy, which was thicker than Au2/PPy and Au3/PPy, and prepared using the potentiostatic deposition step followed by CV deposition step, is shown in Fig. 6. Noteworthy, higher resolution SEM micrographs of Au3/PPy revealed that the microparticles (the largest ones on the surface) are composed of a smaller PPy agglomerates that contain nodular particulates arranged predominantly in a layer by layer fashion.
Fig. 7 CVs of Au2a/PPy preparation in BMIMBF4 (scans 42–100_last) (top), and Au3a/PPY in equimolar BMIMBF4–H2O (scans: 1–21_last) (bottom). |
The two types of polypyrrole electrodes were then characterized by CV and EIS as illustrated in Fig. 8 and 9, respectively. The CV polymer currents recorded in the ionic liquid without added water confirmed a higher yield of polypyrrole prepared with a higher polymerization charge. Therefore, the polymer films (Au1/PPy, Au3/PPy and Au2/PPy) prepared in the first polymerization session can be regarded as thinner (3–4 times) than Au2a/PPy and Au3a/PPy, prepared in the second session. On the other hand, the thinnest film of the second session, Au4a/PPy, has similar thickness to Au2/PPy – the thinnest film of the first session. It is worth to remember that chain length and oxidation degree of polypyrrole was found to decrease with a decrease of the layer thickness.13,18
Fig. 9 EIS spectra of polypyrrole electrodes in BMIMBF4 at +0.2 V: Au2a/PPy , Au3a/PPy , Au4a/PPy . The frequency ranges are indicated above the corresponding complex plane plots. |
The impedance data correlate with the CV data indicating an increase of redox capacitance with charge capacity of the film. In general, the impedance spectra of polypyrrole electrodeposited in the pure salt are similar with the spectra of the polymer prepared with water added to the polymerization bath. However, quantitative differences in the parameter values of the model circuit elements might point out structural dissimilarity of the two kinds of the polymer layers (compare data of Tables 1 and 2). On the other hand, a time parameter of ionic diffusion, B2, being of the order of seconds corresponds to a diffusion coefficient value of the order of 10−8 cm2 s−1 for the polypyrrole samples monitored at 0.2 V by EIS in dry BMIMBF4 at room temperature, irrespective of their preparation history (Au2a/PPy, Au3a/PPy). It is the similar order of D-values as usually found for ionic diffusion in polypyrrole being in contact with molecular aprotic liquid as propylene carbonate12 and in water environment where, however, corresponding D-values are often a little bit lower.11 It should be realized that D-values of the first polymerization session films with thickness of the order of 10−1 μm (Au1/PPy, Au3/PPy) would be of the order of 10−9 cm2 s−1. Surprisingly, the diffusion time parameter couldn't be determined from EIS of the thinnest film, Au4a. Nevertheless, the characteristic diffusion times B2, determined in the presented analysis, do not scale with the film thicknesses. The behavior points out a complex and morphology related diffusion paths.
Parameter/electrode | Au2a/PPy | Au3a/PPy | Au4a/PPy |
---|---|---|---|
R0/kΩ | 1.59 | 0.79 | 0.89 |
1% | 1% | 2% | |
R1/kΩ | 3.98 | 5.49 | 0.265 |
8% | 2% | 5% | |
Y0(Q1)/Ω−1 s+n | 6.1 × 10−6 | 3.1 × 10−6 | 1.4 × 10−6 |
19% | 5% | 12% | |
n(Q1) | 0.58 | 0.78 | 0.69 |
4% | 1% | 1% | |
Y0(Q2)/Ω−1 s+n | 17 × 10−6 | 20 × 10−6 | 5.1 × 10−6 |
8% | 1% | 3% | |
n(Q2) | 0.68 | 0.73 | 0.84 |
2% | <1% | <1% | |
Y0(T)/Ω−1 s+1/2 | 9.9 × 10−6 | 5.5 × 10−6 | — |
5% | 6% | ||
B(T)/s1/2 | 1.9 | 1.8 | — |
3% | 4% |
Importantly, the double layer impedance parameter n1 was found to differ for polypyrrole films bearing different polymerization history: n1 = 0.7–0.8 for the films deposited using the BMIMBF4–H2O mixture (Au3a/PPy and Au4a/PPy), n1 = 0.6 for the BMIMBF4 deposited films Au2/PPy, Au3/PPy, Au1/PPy, and Au2a/PPy.
SEM images of two corresponding polypyrrole layers are shown in Fig. 10.
Fig. 10 SEM micrographs of Au2a/PPy (top) and Au3a/PPy (bottom) deposited using CV in “dry” BMIMBF4 and equimolar BMIMBF4–H2O, respectively, after redox performance in the former electrolyte. |
Polymerization in the mixed solvent, BMIMBF4–H2O, impacts morphology of the polymer film significantly. Even the reference “dry” BMIMBF4 polypyrrole (Au2a/PPY) does not resemble the thinner films prepared during the first session (Au2/PPy, Au3/PPy, Au1/PPY) when the freshly dried ionic liquid was used. The “dry” ionic liquid was dried a few weeks before use and then kept under nitrogen in a closed container stored in a freezer. This ionic liquid as a solvent for polypyrrole deposition resulted in nodular surface structure of the polymer (see Fig. 10 (top)) – generally spherical or irregularly rounded in shape particulates – which is reported as typical morphology for polypyrrole films deposited in different solvents including ionic liquids.16,17,19 Some trace water present in “dry” BMIMBF4 is reasonable explanation for the difference with freshly dried BMIMBF4. This ionic liquid absorbs water from the atmosphere at a fast rate and strong electrostatic field of ions causes hydration of ions thus reducing electrostatic attraction between BMIM+ cation and BF4− anion.21 Thus the liquid crystal like structure of the solvent is distorted by the water molecules and so distribution of dopant ions at a polymerization front is govern by conformation of the flexible polymer chains leading to rounded cauliflower particulates of the polypyrrole phase.
Polymerization in the mixed BMIMBF4–H2O solvent and subsequent processing in “dry” BMIMBF4 resulted in a specific morphology of polypyrrole films (see Fig. 10 (bottom)). Now, polypyrrole films resemble a polydisperse colloid – a dispersion of a solid in a liquid (sol) behaving as a semi rigid mass in which most of the dispersion medium (BMIMBF4) has penetrated into the sol PPy particles forming a gel with some of the dispersed PPy particles visible as islands surrounded by a sea of a rigid liquid. The substantial quantity of water molecules dissolved in BMIMBF4 (1:1) increases the H2O–H2O interactions thus promoting hydrophobic interactions and so adsorption of BMIM+ on gold and polypyrrole. Now again BF4− counterions follow the adsorbed BMIM+ pattern that affects arrangement of PPy chains.
Therefore, the molecular BMIMBF4 surfactant layer formed on gold as well as on electrodeposited polypyrrole is most probably responsible for the specific surface texture of the polymer layer electrodeposited using pyrrole dissolved in the equimolar BMIMBF4–H2O mixed solvent. The crystal-like local structure of the ionic liquid must be highly distorted when the molecular liquid is added. Water added to the BMIMBF4 polymerization solution was in excess of pyrrole for more than 50 times. Molecular films of water miscible imidazolium based ionic liquids on glassy carbon electrodes, formed and applied to electrocatalysis of biological reactants in buffered aqueous solutions, had been already known.22 The equimolar BMIMBF4–H2O electrolyte produces the ionic liquid modified Au electrode by self organization.23 It seems that the BMIMBF4 electrode film in the mixed solvent speeds up the polymerization process by preconcentrating of pyrrole at the modified electrode and causes shorter chains of polypyrrole to dissolve in the ionic liquid. The thinnest polypyrrole layer studied was observed to cover gold by a transparent film. SEM micrographs of Au4a/PPy and Au3a/PPy are similar. However, density of the dispersed solid phase PPy particles is much lower for the thinner Au4a/PPy film (Fig. 11) which may be interpreted as due to the shorter chains of polypyrrole synthesized at the lower potentials.18
Fig. 11 SEM micrograph of Au4a/PPy film prepared by the three steps CV procedure in equimolar BMIMBF4–H2O and later performing in “dry” BMIMBF4. |
The physical properties of aqueous solutions of BMIMBF4 were studied thoroughly in.24 The conductivity–concentration profiles indicate a high degree of aggregation. This ionic liquid is water miscible but its hydrophobicity is manifested by surface tension of the mixture. The surface tension of BMIMBF4–H2O has been shown to be almost constant for the mixtures containing less than 90% (molar) of water. It means the surfactant properties of BMIM+ and tendency to form molecular layers of BMIMBF4 at electrodes. This is certainly the case for our electrodes, Au3a/PPy and Au4a/PPy. Of foremost importance is that no such substantial differences between the mixed solvent, Au3a/PPy, and the ionic liquid, Au2a/PPy, electrodes were observed when characterized by CV and EIS.
Besides the surface activity, ionic liquids based on 1-alkyl-3-methylimidazolium salts in aqueous solution form aggregates that self assembly in a 3D network.25 The bulk structure of BMIMBF4–water mixtures can be of growing importance for morphology of the thicker films of electrodeposited polypyrrole.
Electrochemical impedance spectra showed a highly distributed character of the charge transport processes in all the studied polypyrrole films. In general, the smaller particulates of polypyrrole prepared in water free ionic liquid were shown to enhance the interfacial ion transfer and to impact the bulk film conductance processes by lengthening the diffusion paths. The higher values of the double layer constant phase impedance parameter n(Q1) indicate the more electrically homogeneous surfaces of the semi-rigid polypyrrole films obtained from the mixed solvent. The effective ionic diffusion times do not scale with the polymer film thickness. It points out the morphology related diffusion paths.
It was shown using scanning electron microscopy and energy dispersive X-ray microanalysis that the pure BMIMBF4 and mixed BMIMBF4–H2O electrolytes can be used to tailor the micro and nanostructures of electrodeposited polypyrrole. Submicrometer thicknesses corresponding to microgram amounts of the electrodeposited polymer films were compared through cyclic voltammetry and impedance spectroscopy characteristics of polypyrrole.
Footnote |
† LLP Erasmus 2011/2012 student at University of Wrocław; on leave from Suleyman Demirel University, Chemistry Department, 32260 Isparta, Turkey. E-mail: E-mail: rabiaozsakarya@gmail.com. |
This journal is © The Royal Society of Chemistry 2014 |