Maike Schnucklake*a,
Lysann Kaßnerb,
Michael Mehringb and
Christina Rothc
aInstitute of Chemistry and Biochemistry, Freie Universität Berlin, Arnimallee 22, D-14195 Berlin, Germany. E-mail: maike.schnucklake@fu-berlin.de
bTechnische Universität Chemnitz, Fakultät für Naturwissenschaften, Institut für Chemie, Professur Koordinationschemie, D-09107 Chemnitz, Germany
cElectrochemical Process Engineering, Universität Bayreuth, Universitätsstraße 30, D-95447 Bayreuth, Germany
First published on 18th November 2020
Highly porous carbon–carbon composite electrodes have been synthesized by surface twin polymerization on a macroporous polyacrylonitrile (PAN)-based substrate. For this purpose the compound 2,2′-spirobi[benzo-4H-1,3,2-dioxasiline] (Spiro), being a molecular precursor for phenolic resin and silica, was polymerized onto PAN-based felts with subsequent thermal transformation of the hybrid material-coated felt into silica-containing carbon. The following etching step led to high surface carbon–carbon composite materials, where each carbon component served a different function in the battery electrode: the carbon fiber substrate possesses a high electron conductivity, while the amorphous carbon coating provides the catalytic function. For characterization of the composite materials with respect to structure, porosity and pore size distribution scanning electron microscopy (SEM) as well as nitrogen sorption measurements (BET) were performed. The electrochemical performance of the carbon felts (CF) for application in all-vanadium redox flow batteries was evaluated by cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS). Compared to the pristine PAN-based felt the composite electrodes show significantly enhanced surface areas (up to 35 times higher), which increases the amount of vanadium ions that could be adsorbed onto the surface and thus contributes to an increased performance.
Vanadium redox flow batteries (VRFBs) are a specific type of these batteries, which are already commercialized and readily available. Here, the energy is stored in the form of vanadium-ion containing electrolytes, which consist of V(II)/V(III) at the negative and V(IV)/V(V) at the positive side. The redox reaction takes place at porous, stable, cheap and inert carbon electrodes, which commonly are commercial carbon felts. In general, porous carbon materials are widely used for energy applications, like conversion and storage.14–19 They also recently attracted interest in other fields, such as aeronautics,20,21 hydrogen storage19,22 and biomedical applications,23 where they can be used e.g. for tissue engineering.24 Porous carbon fiber materials satisfy all the requirements for energy applications, including mechanical and thermal strength, as well as relatively low cost.25 However, the poor catalytic activity of carbon felts for the respective redox reactions of the flow batteries is one significant drawback.26 Therefore, one focus of current research is the development of suitable methods for tailoring the felts' properties to enhance their electrochemical performance.27–29 For example Cheng et al. report about the preparation of porous nitrogen doped carbon electrodes derived from biomass.29 Ideal electrodes for use in redox flow batteries should provide high surface area combined with good electrical conductivity and electrochemical stability to facilitate the redox reaction as well as the electron transfer.30
Basically, there exist different strategies to incorporate porosity into carbon materials.31 Due to pyrolysis and subsequent physical or chemical activation of organic precursors, such as wood or coal, porous carbons could be conventionally synthesized. Nowadays, however, the utilization of templates is the most common strategy, as they exert more control on the pore characteristics in the final carbonized product.32 Here, two approaches are equally popular: the hard-templating and the soft-templating method, where in the latter case various surfactants or polymeric detergents are used as structure directing agents.33 During the hard-templating process nanostructured inorganic SiO2 particles are often deployed as porogens, and as a consequence the precursor has to be removed after the carbonization step.31 Both methods generate highly ordered nanostructures with large surface areas.
Spange et al. developed a sophisticated synthesis route called twin polymerization, to produce simultaneously two interpenetrating polymers forming an organic–inorganic hybrid material with only one monomer and one catalyst required.34–39 Moreover, the twin polymerization approach offers several major advantages. As a well-established example the twin monomer 2,2′-spirobi[benzo-4H-1,3,2-dioxasiline] forms phenolic resin and silica without producing any side products, which reduces the shrinking commonly experienced during the stabilization step.36–38,40–42 Ideally, the twin polymerization facilitates the synthesis of nanocomposite domains of 0.5 nm to 3 nm, which is beneficial for the envisaged application.37 It is possible to transform the hybrid materials into highly porous carbon materials by pyrolysis under inert conditions. The silicon dioxide of the hybrid material can serve as an intrinsic template for the porous carbon and can be easily removed by leaching with hydrofluoric acid or sodium hydroxide solution.36–38,42–45 Depending on the choice of the monomer, it is also possible to design the structure of the emerging carbon material. Materials based on the twin monomer Spiro possess micropores which facilitate the adsorption of the redox species, while mesopores are preferentially formed when the precursor tetrafurfuryloxysilane is used. Quantities of monomer, catalyst and substrate can be varied, which allows to develop a huge variety of different porous carbon materials, varying in their properties like porosity and morphology. Furthermore, twin polymerization provides the opportunity to modify the surface of various solid substrates. To obtain a successful coating, the polymerization parameters have to be adapted by considering characteristic features of the used substrate. For example, carbon black as well as Stöber particles were coated by Windberg et al. in this way.45
In 2018, Choudhury et al. used the twin polymerization approach to synthesize a promising carbon cathode for lithium–sulfur batteries.46 Depending on the monomer, which was applied, hollow carbon spheres with microporous or mesoporous shell were synthesized by Böttger-Hiller et al.43 In this study different silicon dioxide particles were used as spherical hard templates to form the porous carbon material. They figured out, that the morphology of the resulting spheres can be influenced by varying the ratio of monomer/substrate and not only by the utilization of different templates. Ebert et al. coated graphite sheets with different layers of amorphous carbon by utilizing the twin polymerization procedure.44 Inspired by these works, we report a synthesis of porous electrode materials for use in redox flow batteries with a significantly increased surface area compared to the state-of-the-art carbon electrodes and with particularly ordered structure. In our preliminary work, highly porous, co-doped composite electrodes were synthesized.47 We demonstrated that the introduction of a greater number of heteroatom-sites enhances the kinetics of the positive half-cell reaction of the redox flow battery. However, it was not possible to differentiate between the effects of the implementation of heteroatoms or the higher surface on the enhanced performance observed for the electrodes.47 Therefore, in this work we focus on the enlargement of the specific surface area without doping the electrode with additional heteroatoms in order to investigate the effect of the increased surface in more detail. With the twin polymerization approach it was possible to produce electrodes, which are suitable for both positive and negative half-cell reactions. The carbon felt structure is used as scaffold with high electron conductivity, whereas the amorphous carbon deposit on its surface should provide the catalytic functionality.
The influence of the catalyst as well as the reproducibility of the twin polymerisation method were investigated and showed that using an acid as catalyst provided a longer lasting stability of the increased electrochemical activity of the electrode. The twin polymerization approach shows a good reproducibility.
Polyacrylonitrile (PAN)-based felts (only stabilized, not yet carbonized) were received from Freudenberg Performance Materials SE & Co. KG (Weinheim, Germany) and utilized as substrate. It should be mentioned here, that the untreated carbon felt is called ‘pristine’. The composite electrodes are named according to the following general scheme – containing the synthesis conditions: material type (catalyst, carbonization time, repeat sequences of etching). The following abbreviations are used for the different catalysts: MSA for acid-catalyzed polymerization and T for thermally induced reaction.
In case of the thermally induced polymerization the felt was given to a solution containing dried DCM (6 mL per 1 g substrate) and 2,2′-spirobi[benzo-4H-1,3,2-dioxasiline] (0.56 g per 1 g substrate). The solution was completely absorbed. After evaporation of the solvent by purging with argon, the felt was heated to 230 °C at a heating rate of 4.1 K min−1 and held at this temperature for one hour in order to carry out the thermally induced polymerization.
For transmission electron microscopy (TEM) analysis, ultra-thin sections of the embedded sample were prepared and investigated with a CM20 FEI instrument.
The specific surface area was measured with an instrument of Quantachrome (Autosorb iQ2) by means of nitrogen adsorption according to Brunauer, Emmett and Teller (BET) with determination of pore size distribution. Before measurement, samples were baked out for 24–48 hours at 80 °C under vacuum (10−4 to 10−5 mbar). In case of the carbon felt electrodes the samples were cut into pieces without grinding and the carbon material was measured as prepared. The specific surface area was calculated by the DFT method and the pore size distributions were determined by applying the nonlocal density functional theory (NLDFT) equilibrium mode method based on slit pores.
Elemental analyses were obtained utilizing the VarioEL Organic Elemental Analyzer from Elementar Analysesysteme GmbH to identify the carbon, hydrogen, nitrogen and sulfur content. The average of the measured values was determined and listed in Table 2.
Thermogravimetric measurements were realized on a Thermogravimetric Analyzer 7 (TGA 7), of PerkinElmer Company (TU Chemnitz, Laboratory of Physical Chemistry). The samples were heated from 30–900 °C with a heating rate of 20 K min−1 under constant air flow. This temperature was held for another 10 to 30 min.
The potentiostatic EIS measurements were implemented in a frequency range from 105 to 10−1 Hz with an AC amplitude of 10 mV and a DC potential of 0.75 V vs. SCE. The EIS data were fitted in the frequency range between 31.25–0.999 Hz and the working electrode was conditioned five minutes at the DC potential before the measurement started.
The carbon material obtained from phenolic resin–silica hybrid material by thermally induced substrate-free twin polymerization is referred to as “carbon material” in the following text, while the synthesized amorphous carbon-coated electrodes are called “composites”.
Additional TEM images of the carbonized, acid-catalyzed sample are given in the ESI (Fig. S1†).
To get rid of the silica phase in the last step of the synthesis procedure, the composite electrodes were etched with an aqueous solution of diluted sodium hydroxide (see Fig. 1). The alkaline treatment was chosen instead of hydrofluoric acid.43,45,46 Choosing this more cautious and environmentally benign approach, it was possible to prevent damage to the composite electrode. Thermogravimetric analysis was selected to test, whether the chosen method was suitable to remove the entire silica template (Fig. 3). During analysis under air, the residue of the TGA analysis gives information about the silicon dioxide content of the evaluated composite material. The composite electrodes show a negligibly small residue of maximum 4.8 wt%, which demonstrates that the template can be removed in an adequate way.
Comparing the curve shapes of the carbonized felt and the composites, it is noticed that the carbonized material loses some water at the beginning, but then appears to be relatively stable. In the differential scanning calorimetry (DSC) curve a sharp endothermic peak is observed at about 700 °C (Fig. 3b). In contrast to that, the curves of the two composite electrodes appear distinctively different. In this case, the first thermolytic degradation already passes through a maximum at around 590 °C, which comes along with a significant mass loss. The two felts have already lost 50% of their mass at approximately 600 °C, while the carbonized sample shows a residual weight of 71 wt% at the respective temperature. Both composite materials show a similar stability. The material obtained by the acidic catalyzed twin polymerization starts to decompose at lower temperatures, while the curve of the composite received by thermally induced polymerization drops slightly faster. Comparison with the DSC curves (Fig. 3b–d) confirms this observation. Here, the endothermic peak of the acidic catalyzed sample seems to be more broadened. In the following it was evaluated whether the composites are stable enough under the conditions of the electrochemical measurements (see Fig. 5).
Nitrogen sorption measurements were conducted to analyze the porosity of the electrode materials and the carbon material. The different curves are shown in Fig. 4a and the respective DFT surface areas are listed in Table 1. The pristine felt shows the typical low surface area of 7 m2 g−1. Compared to the untreated felt, the composite materials show significantly enhanced surface areas (up to 35 times higher), which increases the amount of vanadium ions that could be adsorbed onto the surface. The isotherms of the composite electrodes and the carbon material show furthermore a gas uptake at lower relative pressures indicating a significantly increased contribution from microporosity. For a more detailed insight into the porosity, pore size distributions of the respective materials were calculated and are given in Fig. 4b–d. The corresponding total pore volumes (Vtotal) are listed in Table 1. The composite material, for which the polymerization was thermally induced, as well as its carbon material counterpart present a bimodal distribution with two maxima at a diameter of around 1.5 nm and 4–5 nm. In contrast to that, the reference material exhibits a unimodal distribution with a single maximum in the pore size range higher than 2 nm. It is worth mentioning here, that commercial pristine CFs show predominantly macropores with a literature value of <0.5 m2 g−1.48 Consequently, it is concluded that the micropores are introduced due to the amorphous carbon coating. These assumptions are confirmed by the contributions of the micro- and mesopore volumes to the total volume shown in Table 1. It is evident that the proportion of micropores increases in the order of pristine < carbonized CF < composite (MSA, 1h, E1) < composite (T, 1h, E1) < carbon material (T, 1h, E1) < carbon material (T, 1h, E2) as previously assumed.
DFT surface area/m2 g−1 | Vtotal/cm3 g−1 | (Vmicro) (<2 nm)/cm3 g−1 | (Vmeso) (2–36 nm)/cm3 g−1 | |
---|---|---|---|---|
Pristine | 7 | 0.0156 | 0 | 0.0156 |
Carbonized CF | 43 | 0.06069 | 0.00854 | 0.0521 |
Composite (MSA, 1h, E1) | 123 | 0.1854 | 0.0127 | 0.1727 |
Composite (T, 1h, E1) | 256 | 0.1569 | 0.0764 | 0.0805 |
Carbon material (T, 1h, E1) | 444 | 0.2022 | 0.1495 | 0.0527 |
Carbon material (T, 1h, E2) | 579 | 0.2978 | 0.2081 | 0.0897 |
Depending on the chosen twin monomer, it is possible to tailor the porosity of the resulting carbon. In this case, Spiro was utilized, since the introduction of micropores into the material appears to be beneficial for the intended application.49 It is frequently reported in the literature that a bimodal pore size distribution, in which the micropores facilitate the adsorption and larger mesopores provide fast electrolyte transport, exerts a positive impact on the performance of carbon-based electrodes.50,51
Due to a high amount of white residue in the TGA analysis, which is presumably remaining silicon dioxide, a second etching step of the carbon material became necessary (denoted with suffix E2). By this procedure, the specific surface area was enhanced even further from 444 m2 g−1 to 579 m2 g−1 as a result of further removal of silicon dioxide creating new pores (see Table 1). When looking at Fig. 4b it is striking to see, that an associated increase in microporosity is observed.
Table 2 summarizes the composition of the different carbon electrode materials. All examined samples are mainly composed of carbon, while the pristine felt has a high nitrogen content of 19 wt%, which decreases due to the carbonization step. Note that those values are typical for carbon materials obtained from PAN-based felts, while depending on the starting material the remaining nitrogen content could vary slightly. As intended, both composite materials do not have significantly higher nitrogen contents. Consequently the modification by twin polymerization only produces a coating of porous amorphous carbon material without doping the felts with additional nitrogen. We focused on the positive impact of the enhanced surface area, so that we were able to distinguish between the effect of the doping and the effect of the enhanced surface. Consistent with the aforementioned assumption, the microporous carbon material as received from the substrate-free polymerized monomer has only a negligibly small amount of 0.3 wt% nitrogen. This could be assigned to an impurity from the etching process, since all the nitrogen is contained within the PAN-derived felts.
C/wt% | N/wt% | S/wt% | H/wt% | |
---|---|---|---|---|
a It is worth mentioning here that the residual mass can be attributed to oxygen content or incomplete combustion of the samples.b In accordance with the TGA findings, where we observed a white residue, the residual mass could be attributed to silicon dioxide and additionally from remaining oxygen from the phenolic resin. Oxygen cannot be measured with the chosen approach. | ||||
Pristinea | 58.8 | 19.2 | 0.0 | 4.2 |
Carbonized CF | 91.8 | 5.9 | 0.0 | 0.04 |
Composite (MSA, 1h, E1)b | 81.3 | 6.7 | 0.2 | 0.6 |
Composite (T, 1h, E1)b | 76.5 | 6.7 | 0.0 | 0.3 |
Carbon material (T, 1h, E1)b | 65.7 | 0.3 | 0.0 | 0.3 |
It should be also noted here, that the composite material, for which the polymerization was catalyzed by acid, also contains a small amount of 0.2 wt% of sulfur. This can be attributed to negligible residues of the catalyst material i.e. methanesulfonic acid.
Considering the positive half-cell reaction, it is apparent that both composite materials show a better electrochemical performance as compared to the pristine and the carbonized material. The reversibility of the reaction is significantly improved and a lower peak separation was observed. The maximum currents appear highly symmetric and the onset potentials are shifted to lower potentials for the oxidation and they are shifted to higher potentials for the reduction. In accordance with the nitrogen sorption measurements, the higher surface areas led to an increased double layer capacitance (DLC) in the region between 0.3 V and 0.6 V vs. SCE. The enhanced surface area of the composite is favorable, because due to the additional highly porous carbon material on top of the fibers' surface a higher amount of vanadium ions could be adsorbed. As a result of enhanced surface area, higher maximum currents could be noticed for the composite materials compared to the pristine and the carbonized sample. The composite obtained by acidic catalysis shows the highest maximum currents (see ESI, Table S2†).
Especially, the sample obtained by thermally induced polymerization is characterized by an additional oxidative current at a potential of about 1.0 V (marked with an arrow). Probably, this peak originates from the early onset of corrosion of carbon to carbon dioxide, which was demonstrated in earlier studies with differential electrochemical mass spectrometry (DEMS) measurements.53,54 With higher surface area and higher amount of additional amorphous carbon on the fibers' surface, this oxidative current increases. This observation suggests that the amorphous carbon obtained by the twin polymerization approach is more prone to oxidation. Typically, carbon corrosion in aqueous solution is detected at positive potentials higher than 1.2 V vs. SCE, which gives reason to assume that our amorphous carbon is less stable as compared to commercially routinely-applied carbon material.55 Based on the TGA-analysis, the carbon material also showed lower stability against combustion under air in comparison with the composite electrodes. Here the carbon material already starts to degrade at lower temperatures around 400 °C (see ESI, Fig. S3†). It should be determined, whether this unwanted parasitic carbon corrosion has an impact on the performance of the electrode after several cycles.
The reference material does not show any activity towards the negative redox couple (V(II)/V(III)). Neither an oxidation peak, nor a reduction peak could be observed for the pristine and the carbonized felt. However, the electrodes modified by means of twin polymerization show a good activity for the negative half-cell reaction. This can be seen from two very distinct oxidation- and reduction peaks. The composite, which was polymerized by thermal activation, demonstrates slightly lower maximum currents, while the sample achieved by acidic catalysis shows noticeably stronger evolution of hydrogen. This hydrogen evolution reaction (HER) is known as an undesirable parasitic side reaction,56 which may also be enhanced by an increased specific surface area (marked with an arrow).
Additional electrochemical impedance spectroscopy measurements were performed to study the charge transfer of the V(IV)/V(V) redox reaction. By fitting the EIS data, it was possible to determine the electrical charge transfer resistance and the double-layer capacitance. These are summarized in Table 3 and the corresponding Nyquist plots with utilized equivalent circuit model are shown in the ESI in Fig. S2.†
RCT/Ω | CDL/mF | |
---|---|---|
Carbonized CF | 87.15 | 0.188 |
Composite (MSA, 1h, E1) | 6.363 | 14.34 |
Composite (T, 1h, E1) | 4.369 | 56.06 |
The results for these two parameters fit with our previous assumptions. The carbon coating leads to a larger double-layer capacitance of the electrode/electrolyte interface in agreement with the cyclic voltammetry curves. The charge transfer resistance decreases significantly, which correlates with an accelerated electron transfer. Additionally smaller charge transfer resistances are associated with better kinetics.
The CVs decisively change during the AST test. In case of the composite obtained by acidic catalysis only the maximum current decreases. Here, the peak separation remains unchanged, which means that the reversibility is still good. In contrast to that, the composite synthesized by thermally activated polymerization degrades much faster, which could be seen by a higher peak separation and subsequent DLC decrease after 150 cycles (blue, dashed line; marked by an arrow). In agreement with the recent literature a correlation between the corrosion of carbon and the decrease of the materials surface area could be drawn, which results in a less broadened DLC region.57
It is generally known, that the materials graphitization degree has a significant impact on the corrosion stability, which gives reason to think, that the porous carbon material on top of the fibers is less strongly graphitized.57 For further information about the amount of carbon dioxide produced due the electrochemical corrosion of carbon, differential electrochemical mass spectrometry (DEMS) measurements will be performed in the future. Furthermore, the graphitization degree can be investigated using Raman spectroscopy and the ID:IG ratio as an indication, although one has to consider that Raman spectroscopy is a bulk method, which may have a limited sensitivity to unravel the coating's properties.
It remained to be investigated, if the synthesis is reproducible and provides electrodes with similar activity. For that purpose the synthesis procedure was carried out a second time (see ESI, Fig. S5†). Both obtained material batches show the same activity, whereby the material obtained by the repeated synthesis exhibits slightly increased maximum currents. It is concluded that in this case apparently more porous material could be deposited on the fibers. A slightly increased oxidative current could be also observed, which is in line with the previous results. With increased amount of deposited material on the fibers, the oxidative current increases. This phenomenon will be examined in more detail in the future, to find a way to stabilize the amorphous coating against electrochemical corrosion at higher potentials.
With the twin polymerization approach a porous composite electrode with a significantly increased surface area compared to the state-of-the-art electrodes was obtained, where the porosity of the material can be easily tailored depending on the used twin monomer and the chosen synthesis conditions, such as type of catalysis or maximum temperature. Moreover, a bimodal pore size distribution has been obtained and turned out beneficial for the performance of the electrode facilitating electrolyte transport and accessibility of the active surface. The electrochemical studies showed a significantly increased electrochemical activity and furthermore higher double-layer capacitance for the received material indicating a higher surface area in contact with the electrolyte. In future work, the synthesis will be scaled-up to investigate the composites as electrode materials in full cell battery cycling tests.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0ra07741k |
This journal is © The Royal Society of Chemistry 2020 |