Abstract
Electrolyzers combining CO2 reduction (CO2R) with organic substrate oxidation can produce fuel and chemical feedstocks with a relatively low energy requirement when compared to systems that source electrons from water oxidation. Here, we report an anodic hybrid assembly based on a (2,2,6,6‐tetramethylpiperidin‐1‐yl)oxyl (TEMPO) electrocatalyst modified with a silatrane‐anchor (STEMPO), which is covalently immobilized on a mesoporous indium tin oxide (mesoITO) scaffold for efficient alcohol oxidation (AlcOx). This molecular anode was subsequently combined with a cathode consisting of a polymeric cobalt phthalocyanine on carbon nanotubes to construct a hybrid, precious‐metal‐free coupled AlcOx–CO2R electrolyzer. After three‐hour electrolysis, glycerol is selectively oxidized to glyceraldehyde with a turnover number (TON) of ≈1000 and Faradaic efficiency (FE) of 83 %. The cathode generated a stoichiometric amount of syngas with a CO:H2 ratio of 1.25±0.25 and an overall cobalt‐based TON of 894 with a FE of 82 %. This prototype device inspires the design and implementation of nonconventional strategies for coupling CO2R to less energy demanding, and value‐added, oxidative chemistry.
Keywords: alcohols, carbon dioxide, catalyst immobilization, electrocatalysis, energy conversion
Inspirational device: A molecularly engineered electrolyzer was constructed for the selective oxidation of glycerol to glyceraldehyde, with a turnover number (TON) of ≈1000 and a Faradaic efficiency (FE) of 83 %, coupled with aqueous CO2 reduction to generate a stoichiometric amount of syngas, with a CO:H2 ratio of 1.25±0.25, an overall TON of 894 and FE of 82 %.
Introduction
The electrosynthesis of fuels is being pursued as a potential solution to intermittent electricity production via renewable wind and solar technologies.1 Conventional fuel‐generating electrolyzers couple the oxygen evolution reaction (OER) at the anode to the hydrogen evolution reaction (HER) or CO2R at the cathode.2, 3 However, the kinetic hurdles of the anodic four‐electron process and consequently large overpotential for the OER, tied to the limited commercial value of O2, are spurring interest in employing more synthetically useful and facile organic oxidative reactions.4, 5, 6, 7, 8, 9, 10, 11
Recent technoeconomic studies have shown that ≈90 % of the overall energy requirements for current commercial approaches in CO2 electrolysis stem from the OER, and that lower cell potentials for fuel‐generating reductive chemistry can be achieved by substituting the OER for AlcOx.12 In particular, by combining theory and experiment, it was shown that glycerol, a biomass‐derived platform chemical and a by‐product from the production of biodiesel and soap,13, 14 is an attractive candidate that can greatly improve the economics of the overall redox process.
Reports on dual AlcOx–CO2R electrolyzers suffer from two main drawbacks to date.7, 9 Firstly, precious metal‐containing components are employed in the electrolysis cells. Secondly, homogeneous catalysts and mediators are required in excess in the electrolyte solution, which complicates post‐reaction processing of the liquid products. The use of dissolved catalysts presents an additional challenge during electrosynthesis, because only a tiny fraction of the catalyst (positioned in the Helmholtz layer) can turnover, while the rest remains inactive in the bulk solution.
Here, we consider glycerol as a commercially viable resource to develop a robust and precious‐metal‐free anodic assembly for coupling with the cathodic CO2R reaction. We modified TEMPO, an efficient, non‐toxic, molecular (electro)catalyst that can oxidize a wide range of alcohol substrates under mild conditions,15, 16 with a silatrane anchor (giving STEMPO), for robust immobilization on a mesoITO scaffold (Figure 1). The porous electrode enables high catalyst loading, while the immobilization procedure permits direct electronic communication between the electrode and the molecular species, leading to constant catalytic turnover, easier product isolation and catalyst recyclability. The performance of the mesoITO|STEMPO assembly was assessed under different conditions with a range of alcohols.
We then coupled the anode to a hybrid CO2R cathode, featuring a cobalt phthalocyanine (CoPc) based electrocatalyst. CoPc was polymerized onto carbon nanotubes (CNTs) to form a CNT‐polymeric CoPc composite (CNT‐CoPPc; where CoPPc denotes polymeric cobalt phthalocyanine), which was then deposited onto porous carbon paper (CP, cathode assembly henceforth denoted as CP|CNT‐CoPPc)17 (Figure 1). The AlcOx–CO2R electrolyzer oxidizes glycerol to glyceraldehyde with good catalytic performance and high selectivity, and generates a stoichiometric amount of syngas at the cathode.
Results and Discussion
Metal oxide (MOx) electrodes present a suitable platform for catalyst immobilization as they offer affinity for a variety of anchoring units, and the possibility to morphologically tune the surface to enhance the loading of molecular components.18, 19 Metal oxides can exhibit different electronic properties, as demonstrated by the metallic behavior of ITO and the semiconductive properties of TiO2, thus offering a versatile electroactive platform to combine with surface‐anchored molecular catalysts.20, 21 Several mechanistic studies have highlighted the effect of pH on the TEMPO catalytic cycle, with enhanced oxidation rates observed under more basic conditions.22, 23, 24 This stringent criterion implies that some of the more commonly used anchoring groups compatible with MOx scaffolds, such as carboxylic acids and phosphonic acids (pH stability <4 and 7, respectively),25 may not be suitable for TEMPO immobilization on an ITO electrode. We therefore designed STEMPO, which contains a caged silatrane unit to improve binding to the MOx. The silatrane moiety can hydrolyze on the MOx surface to form strong siloxane bonds, which provide an increased anchor stability under more alkaline conditions (Figure 1).26, 27
STEMPO was synthesized in good yield by reacting the acyl chloride of 4‐carboxy‐TEMPO with 3‐aminopropylsilatrane. Full synthetic and characterization details (high‐resolution mass spectrometry, infrared spectroscopy (Figure S1) and elemental analysis) are provided in the Supporting Information.
The mesoITO|STEMPO anode was assembled by incubating the mesoITO electrode (film thickness ≈4.5 μm, Figure S2) in a solvent bath mixture containing STEMPO, and heating the solution to 70 °C under a N2 atmosphere for 6 h. Multi‐scan cyclic voltammetry (CV) measurements were used to deduce the optimal mixture, in which the surface loading of STEMPO (ΓSTEMPO) on the mesoITO scaffold was both maximal and stable, with ΓSTEMPO being determined by integrating the charge passed in the oxidation wave of the consecutive cyclic voltammograms (see Supporting Information, Equation (S1)). The best mixture consisted of a STEMPO solution (2 mm) with 2 %(v/v) acetic acid (AcOH) and 1 %(v/v) H2O in acetonitrile (MeCN). With regards to the stability of the immobilized STEMPO compound, MeCN was the most suitable solvent from those attempted (Figure S3). The combination of AcOH and H2O facilitated the hydrolysis of the silatrane cage on the mesoITO surface,28 and was deemed necessary for instigating the anchoring process (Figure S4 and S5). Optimal ΓSTEMPO was typically found to be 20–25 nmol cm−2, which is in the expected range for nanostructured ITO surfaces.29, 30
X‐ray photoelectron spectroscopy (XPS) showed binding signals in the Si2p and N1s regions (Figure 2 a and Figure S6, respectively), where the Si2p signal agrees with XPS reference spectra for the siloxane‐bearing group.31
Multiple CV scans of the mesoITO|STEMPO electrode reveal a reversible redox wave at E 1/2=0.83 V vs. NHE (Figure 2 b), which corresponds to the nitroxide/oxoammonium species, and is only slightly more positive than that of dissolved TEMPO (E 1/2=0.74 V vs. NHE, Figure S7a). At low scan rate (10 mV s−1), the peak‐to‐peak separation is below 20 mV and is thus in good agreement with the ideal value of 0 mV for a reversible response of a surface‐adsorbed species (Figure S7b). The full width at half‐maximum is 116 mV (Figure S7b), only slightly broader than the theoretically predicted value of around 91 mV for a 1 e− process (at 25 °C).32 This slight deviation from ideal behavior can be attributed to multilayer formation,33, 34 stemming from the cross‐polymerization of Si‐O‐Si bonds between adjacent anchoring units in the mesoporous scaffold and film resistance of the mesoITO electrode.
A deeper analysis of the electron‐transfer dynamics of the mesoITO|STEMPO system was inferred using the Laviron method,35 which relies on the change in the peak potential (ΔE p) with scan rate (ν). The resulting trumpet plot for the mesoITO|STEMPO assembly is portrayed in Figure 2 c. The intercepts of the linear regions of the plot can be used to deduce the critical scan rate (ν c) and the apparent electron transfer rate constant (k app) for the system (see Supporting Information for further details). Values for ν c and k app were determined to be equal to 72±2 mV s−1 and 0.68±0.02 s−1, respectively. The rate of electron transfer appears to be low (hence the low value for ν c), but is comparable with other covalently linked redox species in the literature.36 Figure S8 depicts the CV scans measured over a range of scan rates to highlight the change in the peak‐to‐peak separation for the STEMPO redox wave as the applied scan rate exceeds ν c. The linear relationship between the peak current (i p) and ν, for ν<ν c (Figure 2 d), is characteristic for a surface‐immobilized redox entity.32 The pH stability of the mesoITO|STEMPO assembly was investigated using a multi‐scan CV approach, whereby the electrode was subjected to several redox cycles in solutions of differing pH (Figure 2 e and Figure S9). A good stability was obtained after 200 scans at pH 7 and 8 (decrease in signal intensity of 34 % and 39 %, respectively, relative to scan 1), and the decay curve only began to be more severe at pH 10. These results support that the assembly is suited to operate under the basic conditions required for enhanced TEMPO catalysis.
Immobilization and direct wiring of STEMPO to the mesoITO electrode was confirmed by film electrochemical electron paramagnetic resonance (FE‐EPR) spectroscopy (see Supporting Information).37 The combined FE‐EPR spectroelectrochemical technique allows for the appearance and disappearance of paramagnetic species to be monitored as a function of the applied potential in the absence of any mediators. The high electrical conductivity combined with the surface‐modification properties of ITO make it a suitable platform for carrying out FE‐EPR spectroscopy. Carbon‐based electrodes tend to give rise to large radical signals and are thus unsuitable for such studies.37
For FE‐EPR spectroscopy, cylindrical mesoITO (C‐mesoITO) electrodes were employed for use in the EPR spectroelectrochemical cell. The unpaired electron in the TEMPO moiety is delocalized around the N and O atoms with nuclear spins (I) of 1 and 0, respectively, and thus only couples with N nuclei. This interaction gives rise to a triplet pattern in which the peaks, for the case of a diffusional species tumbling rapidly in solution at room temperature, are all the same intensity (EPR spectrum for diffusional TEMPO presented in Figure S10a, black trace). A triplet pattern is also discernible for the C‐mesoITO|STEMPO assembly, but the peak intensities are distorted in this case (Figure S10a, red trace). This change in line‐shape of the EPR spectrum relative to the diffusional case arises from a slower tumbling rate which can be a consequence of the impaired mobility of the TEMPO moiety upon STEMPO immobilization.38
Figure 2 f highlights the results from the FE‐EPR investigation. C‐mesoITO|STEMPO samples were poised at a particular potential, using a three‐electrode setup, and then flash‐frozen to allow for low‐temperature EPR characterization. Examples of EPR spectra, at three different potentials, are presented in Figure 2 f (inset) (full range in Figure S10b), where an increase in the applied bias is accompanied by a drop in signal intensity, that eventually vanishes due to the oxidation of the radical to EPR‐silent STEMPO +. The shape of the EPR spectra for E<1.0 V vs. NHE are typical of nitroxide radicals measured at low temperatures (100 K).39 The normalized signal area of each individual EPR spectrum was plotted as a function of the potential, and is a close fit to the anticipated 1 e− Nernst equation (solid line, Figure 2 f).
Next, we investigated the catalytic performance of the mesoITO|STEMPO assembly. Figure 3 a depicts the catalytic behavior of the system as a function of the solution pH, where 4‐methylbenzyl alcohol (MBA) was chosen as a model substrate. The current density increases with increasing pH, accompanied by a lower onset potential for catalysis (from 0.75 V at pH 7.3, to 0.68 V at pH 10, vs. NHE), which is comparable to previous reports for immobilized TEMPO on carbon‐based electrodes.40, 41 This observation is in‐line with the established TEMPO‐mediated oxidation mechanism, whereby alcohol deprotonation leads to formation of a pre‐oxidation complex via nucleophilic attack of the alkoxide on the electrophilic nitrogen of the oxidized TEMPO moiety (the oxoammonium cation), prior to aldehyde formation.24, 41, 42, 43 However, the enhancement starts to plateau between pH 9 and pH 10, contrary to what is observed for TEMPO, and related nitroxyl derivatives, in solution.43 The plateau shown in Figure 3 a for the mesoITO|STEMPO system could be due to a combination of factors, and we rationalize this behavior to stem from the relatively slow electron transfer between the ITO electrode and immobilized STEMPO, as well as from mass transport limitations of the substrate in the mesoporous film.
Controlled potential electrolysis (CPE) was then conducted at an applied potential (E app) of 1.0 V vs. NHE at room temperature, to further probe the effect of pH on the mesoITO|STEMPO system. Figure 2 e shows that the stability of the anodic, molecular assembly is high at pH 7 and 8, but less so at pH 10. However, the TEMPO‐mediated catalysis, and hence reaction kinetics, are favored under more alkaline conditions (Figure 3 a). To compare the overall mesoITO|STEMPO performance as a function of pH, the TON and FE (Supporting Information, Equations (S4) and (S5), respectively) were calculated after a 3 h CPE experiment with MBA (30 mm) as the substrate, at four different pH values (Figure 3 b, Figure S11). The moles of product, 4‐methylbenzaldehyde (n MBAd), originating from selective MBA oxidation, were quantified by high performance liquid chromatography (HPLC) (Supporting Information).
The TON for STEMPO experiences a maximum at pH 8, reaching a value close to 3000, highlighting the fine balance between immobilization stability and catalytic activity in long‐term electrolysis experiments. On either side of the maximum, there is a corresponding decrease in the TON. At lower pH, this can be attributed to a lower rate of substrate oxidation thereby resulting in less n MBAd, whereas higher pH adversely affects the stability of the mesoITO|STEMPO assembly, likely leading to a loss of the catalytic sites from the electrode over reaction time. Post‐CPE (at pH 8) XPS conducted on the mesoITO|STEMPO electrode reveals peaks in the Si2p and N1s regions (Figure S12), similar to those observed on a freshly assembled electrode (Figure 2 a and Figure S6), and thus indicates that the gradual drop in activity could be primarily due to hydrolysis of the amide bond and subsequent loss of the TEMPO moiety from the assembly. On the other hand, the FE is invariant with the pH (average of 86±3 % as calculated across the pH range, Figure 3 b), implying that the charge passed at the electrode|catalyst interface is utilized in the same, selective manner (being directed towards substrate oxidation) throughout the pH range.
The versatility of the hybrid electrode was demonstrated by extending the substrate scope to glycerol, cellulose‐derived hydroxymethylfurfural (HMF), and the lignin model compound 2‐phenoxy‐1‐phenylethanol (PP‐ol; Table S2).44 A turnover frequency (TOF) analysis based on the sigmoidal catalytic response of the CV trace was performed for the STEMPO system in the presence of the different substrates (Supporting Information).45 Figures 3 c and 3d depict concentration profiles obtained for glycerol and HMF, respectively, and the concentration profile for MBA is shown in Figure S13a (corresponding “maximum current density vs. concentration” plots for these three substrates are presented in Figure S13b–d). PP‐ol was poorly soluble in pure aqueous electrolyte, and thus a CV trace for this compound was recorded in a MeCN–water mixture (Figure S14). The estimated TOFs for the four compounds, and the relevant experimental conditions, are summarized in Table S2. The results show that the mesoITO|STEMPO system can be used to oxidize a variety of alcohol‐based substrates, with the primary benzylic alcohols MBA and HMF showing the highest activity (TOF=0.677 and 0.680 s−1, respectively), followed by the aliphatic triol, glycerol (0.557 s−1). The results from this analysis therefore encourage the use of low‐cost and abundant alcohols such as glycerol for electrocatalytic applications with the mesoITO|STEMPO electrode. PP‐ol gave the lowest TOF (0.268 s−1), which agrees with the expected trend that primary alcohols are oxidized more rapidly than secondary alcohols by TEMPO in basic solution.42
Having characterized the anodic assembly and demonstrated the electrocatalytic compatibility of mesoITO|STEMPO with a variety of biomass representative alcohols, we turned towards applying this system within a coupled electrolyzer. Conversion of CO2‐to‐syngas as the cathodic half‐reaction presents an attractive strategy to utilize the electrons from alcohol oxidation by mesoITO|STEMPO. To facilitate a cost‐efficient redox cycle, use of robust, earth‐abundant catalysts for selective CO2R is essential. While many 3d transition metal‐based molecular catalysts have been developed over the years,46 CoPc has emerged as one of the most promising catalysts for CO2‐to‐CO reduction because of its enhanced performance upon immobilization onto polymers and carbon‐based electrodes.47, 48, 49 In the coupled electrolyzer, we employed a CNT‐CoPPc hybrid, fabricated by in situ polymerization, that was subsequently deposited on CP.17 The CP|CNT‐CoPPc cathode catalyzes the electrochemical reduction of CO2 to syngas, with a CO:H2 ratio dependent on the applied potential.17, 50
The CV trace recorded for CP|CNT‐CoPPc under N2 displays a broad quasi‐reversible redox process (Figure 4 a, E 1/2≈−0.71 V vs. NHE), which corresponds to the metal‐centered CoII/CoI reduction of CoPPc. The surface concentration of electroactive cobalt centers was estimated to be 18.3±1.6 nmol cm−2 from integration of the CoI/CoII oxidation wave (Figure S15). This corresponds to 5.6±0.5 % cobalt sites being electrochemically accessible, whereby the total amount of Co was determined using inductively coupled plasma optical emission spectroscopy (ICP‐OES) measurements (Supporting Information, Eq. (S6)).
A catalytic onset from the CP|CNT‐CoPPc electrode was observed in a CO2‐saturated solution at a potential close to −0.84 V vs. NHE (Figure 4 a). Electrocatalytic performance of the cathode was probed by stepped constant potential chronoamperometry in the range of −0.70 to −1.00 V vs. NHE, with 50 mV increments and 30 min steps (Figure S16). Product formation was monitored via a continuous flow gas chromatography (GC) method (Supporting Information). H2 was the only product until −0.80 V vs. NHE and CO evolution started at more negative potentials (≈−0.85 V vs. NHE). The selectivity of the electrode towards CO increases sharply at more negative potentials, reaching 76 % at −1.00 V vs. NHE (overpotential, η=0.46 V, where E(CO2/CO)=−0.54 V vs. NHE at pH 7.3).51 Within the same potential range, the blank CNT electrode did not generate any H2 or CO (Figure S16a, purple trace).
To elucidate the working principle of the coupled mesoITO|STEMPO–CP|CNT‐CoPPc electrolyzer, initial experiments were conducted using MBA. A catalytic wave for the mesoITO|STEMPO assembly in the presence of MBA (30 mm) was observed, which appeared to plateau at around 3 mA cm−2, at an applied potential just above 1 V vs. NHE (Figure 4 b). The mesoITO|STEMPO electrode displayed slightly lower current densities than CP|CNT‐CoPPc and was therefore selected as the working electrode (WE) in the coupled electrolyzer, while the cathode assumed the role of the counter electrode (CE). A two‐compartment electrochemical cell was employed with a Selemion‐AMV anion‐exchange membrane to separate the compartments. A Ag/AgCl reference electrode (RE) was placed in the working compartment and the three‐electrode configuration was adopted prior to studying a two‐electrode system, to be able to precisely control the E app at the WE versus a known reference (Supporting Information). This also allowed us to record the exact potential at the CE (E CE) during electrolysis against the same reference, thus providing a more detailed description of the cell parameters over reaction time.
A CO2‐saturated carbonate buffer (0.5 m) was used in both compartments, which yielded a solution pH close to 7.3 that remained relatively constant throughout the experiment. Figure 4 c depicts the results from the coupled electrolysis (three‐electrode configuration), with E app=1.0 V vs. NHE at room temperature. Alcohol conversion to the corresponding aldehyde, MBAd, was quantified by HPLC, whereas CO and H2 were quantified by a continuous flow GC method (Supporting Information). Catalytic metrics obtained for the respective anode and cathode highlight the effectiveness of the combined system. MBA oxidation resulted in a TONSTEMPO of 1515 and FE close to 90 % after the 3 h CPE experiment. The TONSTEMPO was lower than expected from the TOF analysis from CV scans (Table S2) due to the modest stability of the anodic assembly, as demonstrated by the multiple CV scan measurements and prolonged CPE (cf. Figure 2 e and Figure 3 b, respectively). A cobalt‐based TON for syngas generation of 1360 (TONCO=599 and TON =761) and overall FEs for CO and H2 of 35 % and 45 %, respectively, were achieved for the CP|CNT‐CoPPc cathode.
This performance encouraged the substitution of MBA for glycerol, on account of its advantages as a potential substrate for coupling with CO2R in ‘real‐life’ applications. A similar setup to that used for coupled MBA oxidation was employed, except in this case, the anode compartment consisted of a carbonate buffer (0.5 m) at pH 8.3 (under N2), whereas the catholyte was comprised of a CO2 saturated carbonate buffer (0.5 m) at pH 7.3. This was deemed necessary for glycerol, as the STEMPO‐mediated catalysis involving this substrate was observed to be too sluggish at the quasi‐neutral pH of CO2‐saturated carbonate buffer (i.e. pH 7.3), but increased in activity under more alkaline conditions (as evidenced by the CVs recorded at pH 7.3 and 8.3, Figure S17). Figure 5 a illustrates the reaction time plot obtained with glycerol as the substrate, with E app=1.0 V vs. NHE. HPLC analysis revealed that glyceraldehyde (GlyAd) was the primary anodic product from the coupled electrolysis experiment.
The two compartments maintained their individual pH values for the duration of the electrolysis, and a TONSTEMPO and FE of 997 and 83 %, respectively, were measured for the anodic half‐reaction. Although precautions were taken to minimize overoxidation or further reaction of GlyAd, trace amounts of some side‐product can potentially form (not detected by HPLC), leading to the observed ≈7 % drop in the FE relative to the MBA electrolyzer. With regards to the cathode metrics, the cobalt‐based TON was determined to be equal to 894 (TONCO=444 and TON =450), while similar FEs for the gaseous products, relative to the MBA‐based electrolyzer, were measured (FE=41 % for CO, 41 % for H2). A side‐by‐side comparison of the calculated FEs for the liquid and gaseous products over reaction time, for the MBA‐ and glycerol‐based electrolyzers, is provided in the Supporting Information (Figure S18).
The three‐electrode configuration allowed for E CE (i.e. the potential at the CP|CNT‐CoPPc electrode) to be monitored throughout the course of the electrolysis experiment. From the traces shown in Figure 5 b, there is an alteration in the CO:H2 ratio at the cathode over time, which seems to reflect the change in E CE. This decrease in the reducing potential at the cathode is itself a result of the gradual decline in activity at the anode over time. The change in the CO:H2 ratio as a function of the cathodic potential is in‐line with the stepped chronoamperometric experiments carried out for the CP|CNT‐CoPPc electrode (with Pt mesh as CE), as discussed above (Figure S16). The time‐lag between the minima of the E CE trace and the maximum value of CO:H2 ratio on Figure 5 b is likely caused by the slow diffusion of CO from the porous cathode.
We furthered our investigation into coupled glycerol oxidation and CO2R, and performed a series of experiments in a more practical two‐electrode configuration, while varying the applied cell potential (V cell). Values for V cell in the range of 1.8 to 2.1 V were chosen, based on the rationale that: |E cathode−E anode|≈| −E app|=1.85 V, where is the average potential at the CE, over reaction time, as measured in the three‐electrode configuration (i.e. Figure 5 b). Figure 5 c depicts the combined FE at the cathode (for CO and H2) and the CO:H2 ratio, over reaction time, for V cell=2.0 V. The trends agree with those obtained for the three‐electrode setup. The increase in the maximum of the CO:H2 ratio for the two‐ versus three‐electrode configuration (shown in Figure 5 b) could be a result of the increased driving force provided by the 2.0 V potential. This bias most likely leads to more reductive potentials at the cathode, and, in accordance with the stepped chronoamperometry data for CP|CNT‐CoPPc (Figure S16), would translate to a higher CO:H2 ratio.
Finally, we calculated the cell energy efficiency (ϵ), as a function of V cell using Equation (1):12
(1) |
where , , and E GlyAd/glycerol denote the reduction potentials for H+, CO2, and glyceraldehyde, respectively, under non‐standard conditions (Table S3). A more detailed breakdown regarding the thermodynamic analysis required to compute ϵ is provided in the Supporting Information. Figure 5 d illustrates the FEs for the anodic and cathodic processes, along with the corresponding ϵ calculations, for different V cell values. There is a slight improvement in the CO selectivity upon increasing from 1.8 to 1.9 V (FECO=36 and 46 %, respectively), presumably a result of the higher driving force at these applied voltages. This enhancement is met with an improvement in ϵ (from 16 to 18 %), since the 100 mV additional bias is offset by the increase in FECO, as governed by Equation (1). However, for V cell≥2.0 V, the combined effects of a largely unchanged CO:H2 ratio and anodic FE, causes a corresponding drop in the cell efficiency to ≈16 %, similar to that obtained for V cell=1.8 V. The cell energy efficiency values measured for our hybrid electrolyzer are in accordance with those reported in the literature, where for example an efficiency of 17 %, at 1.8 V cell potential, was measured for a dual electrolyzer featuring benzyl alcohol oxidation coupled with the reduction of aqueous CO2 to CO and H2.9 However, the previously reported system was comprised of Ru‐based molecular catalysts for the reductive and oxidative half‐reactions, and additionally, only one of the catalysts was immobilized. In contrast, we have incorporated immobilized cathodic and anodic catalysts in our electrolyzer, both free of any precious metals, and have also demonstrated the applicability of the tandem AlcOx–CO2R device to couple the oxidation of more commercially viable substrates, such as glycerol, with CO2‐to‐syngas conversion.
Conclusion
We have designed, fabricated and characterized an anode featuring a silatrane‐modified TEMPO molecule on a mesoITO scaffold, and demonstrated the electrocatalytic ability of the molecularly engineered MOx system to efficiently oxidize a variety of biomass representative substrates. The siloxane anchor, formed upon hydrolysis of the silatrane cage on the MOx surface, displays robust binding. The catalytically active site (i.e. the oxoammonium cation) is both stable and readily regenerated under electrocatalytic conditions,52 and we believe that the long‐term stability of the hybrid electrode assembly is currently limited by the amide bond in STEMPO. Improvements to the molecular design of the linker employed for STEMPO will provide a possibility to enhance the stability and overall activity of the anodic assembly.
We further showed the advantage and versatility of our novel STEMPO anode by coupling alcohol oxidation with an efficient CO2R cathode (CP|CNT‐CoPPc), to construct an AlcOx–CO2R electrolyzer based on immobilized, precious‐metal‐free, ‘molecular’ catalysts. The functionality and performance of the device was investigated using a three‐electrode configuration, first employing MBA as a model substrate, and later, using the commercially applicable substrate, glycerol. It was found that in both cases, stoichiometric amounts of a selective oxidation product (the corresponding aldehyde) and syngas were generated at the anode and cathode, respectively. FEs were typically excellent for the hybrid system, exceeding 80 % for both anode and cathode. TONs were also high, approaching 1000 for mesoITO|STEMPO and 900 for CP|CNT‐CoPPc (with glycerol as substrate). The TON of the cathode in the electrolyzer is currently limited by the prolonged stability issue of the anodic assembly during continuous CPE experiments and the CoPPc‐cathode on its own is known to maintain activity over a longer time‐period.17 Further studies were then made using a demonstrator‐type, two‐electrode setup for coupled glycerol oxidation at the anode and syngas generation at the cathode, showing similar performance metrics as the three‐electrode system. Cell energy efficiency calculations also revealed the advantages of operating at a lower V cell, with a maximum efficiency of 18 % being measured at a cell potential of 1.9 V. This molecular hybrid system is therefore a suitable model for the development of future AlcOx–CO2R electrolyzers based on earth‐abundant materials, which can provide chemical feedstocks (aldehydes and syngas) from sustainable and abundant resources, such as biomass‐derived alcohols, CO2, and renewable electricity.
Conflict of interest
The authors declare no conflict of interest.
Supporting information
Acknowledgements
This work was supported by the Endeavour Scholarship Scheme (M.B.), the Christian Doppler Research Association (Austrian Federal Ministry for Digital and Economic Affairs and the National Foundation for Research, Technology and Development), OMV (M.A.B., J.W., A.W., E.R.), a Marie Skłodowska‐Curie Fellowship from the European Commission H2020 (S.R., GAN745604, CO2RED), the Leverhulme Trust (M.M.R & E.R, RPG‐2018‐183), and the EPRSC (EP/L011972/1 to CAESR). The authors thank Dr. Christian Pichler for assistance with HPLC measurements, Mr. Adam Brown for XPS measurements, Dr. Bertrand Reuillard, Dr. Qian Wang and Dr. Sam Cobb for helpful discussions, and the Centre for Advanced ESR (University of Oxford) for EPR measurement time.
M. A. Bajada, S. Roy, J. Warnan, K. Abdiaziz, A. Wagner, M. M. Roessler, E. Reisner, Angew. Chem. Int. Ed. 2020, 59, 15633.
References
- 1. De Luna P., Hahn C., Higgins D., Jaffer S. A., Jaramillo T. F., Sargent E. H., Science 2019, 364, eaav3506. [DOI] [PubMed] [Google Scholar]
- 2. Kang P., Chen Z., Nayak A., Zhang S., Meyer T. J., Energy Environ. Sci. 2014, 7, 4007–4012. [Google Scholar]
- 3. McCrory C. C. L., Jung S., Ferrer I. M., Chatman S. M., Peters J. C., Jaramillo T. F., J. Am. Chem. Soc. 2015, 137, 4347–4357. [DOI] [PubMed] [Google Scholar]
- 4. Cha H. G., Choi K.-S., Nat. Chem. 2015, 7, 328–333. [DOI] [PubMed] [Google Scholar]
- 5. Horn E. J., Rosen B. R., Chen Y., Tang J., Chen K., Eastgate M. D., Baran P. S., Nature 2016, 533, 77–81. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 6. You B., Liu X., Jiang N., Sun Y., J. Am. Chem. Soc. 2016, 138, 13639–13646. [DOI] [PubMed] [Google Scholar]
- 7. Li T., Cao Y., He J., Berlinguette C. P., ACS Cent. Sci. 2017, 3, 778–783. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 8. Li T., Kasahara T., He J., Dettelbach K. E., Sammis G. M., Berlinguette C. P., Nat. Commun. 2017, 8, 390. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 9. Wang Y., Gonell S., Mathiyazhagan U. R., Liu Y., Wang D., Miller A. J. M., Meyer T. J., ACS Appl. Energy Mater. 2019, 2, 97–101. [Google Scholar]
- 10. Huang C., Huang Y., Liu C., Yu Y., Zhang B., Angew. Chem. Int. Ed. 2019, 58, 12014–12017; [DOI] [PubMed] [Google Scholar]; Angew. Chem. 2019, 131, 12142–12145. [Google Scholar]
- 11. Reisner E., Angew. Chem. Int. Ed. 2019, 58, 3656–3657; [DOI] [PubMed] [Google Scholar]; Angew. Chem. 2019, 131, 3694–3695. [Google Scholar]
- 12. Verma S., Lu S., Kenis P. J. A., Nat. Energy 2019, 4, 466–474. [Google Scholar]
- 13. Yazdani S. S., Gonzalez R., Curr. Opin. Biotechnol. 2007, 18, 213–219. [DOI] [PubMed] [Google Scholar]
- 14. Dai C., Sun L., Liao H., Khezri B., Webster R. D., Fisher A. C., Xu Z. J., J. Catal. 2017, 356, 14–21. [Google Scholar]
- 15. Semmelhack M. F., Schmid C. R., J. Am. Chem. Soc. 1983, 105, 6732–6734. [Google Scholar]
- 16. Miyazawa T., Endo T., Shiihashi S., Okawara M., J. Org. Chem. 1985, 50, 1332–1334. [Google Scholar]
- 17. Han N., Wang Y., Ma L., Wen J., Li J., Zheng H., Nie K., Wang X., Zhao F., Li Y., et al., Chem 2017, 3, 652–664. [Google Scholar]
- 18. Hoertz P. G., Chen Z., Kent C. A., Meyer T. J., Inorg. Chem. 2010, 49, 8179–8181. [DOI] [PubMed] [Google Scholar]
- 19. Mersch D., Lee C. Y., Zhang J. Z., Brinkert K., Fontecilla-Camps J. C., Rutherford A. W., Reisner E., J. Am. Chem. Soc. 2015, 137, 8541–8549. [DOI] [PubMed] [Google Scholar]
- 20. Rosser T. E., Windle C. D., Reisner E., Angew. Chem. Int. Ed. 2016, 55, 7388–7392; [DOI] [PMC free article] [PubMed] [Google Scholar]; Angew. Chem. 2016, 128, 7514–7518. [Google Scholar]
- 21. Rosser T. E., Reisner E., ACS Catal. 2017, 7, 3131–3141. [Google Scholar]
- 22. Bobbitt J. M., Brückner C., Merbouh N., in Organic Reactions, Vol 74 (Ed. S. E. Denmark) Wiley, Hoboken, NJ, 2010, pp. 103–424. [Google Scholar]
- 23. Rafiee M., Karimi B., Alizadeh S., ChemElectroChem 2014, 1, 455–462. [Google Scholar]
- 24. Hickey D. P., Schiedler D. A., Matanovic I., Doan P. V., Atanassov P., Minteer S. D., Sigman M. S., J. Am. Chem. Soc. 2015, 137, 16179–16186. [DOI] [PubMed] [Google Scholar]
- 25. Materna K. L., Crabtree R. H., Brudvig G. W., Chem. Soc. Rev. 2017, 46, 6099–6110. [DOI] [PubMed] [Google Scholar]
- 26. Brennan B. J., Llansola Portolés M. J., Liddell P. A., Moore T. A., Moore A. L., Gust D., Phys. Chem. Chem. Phys. 2013, 15, 16605–16614. [DOI] [PubMed] [Google Scholar]
- 27. Materna K. L., Brennan B. J., Brudvig G. W., Dalton Trans. 2015, 44, 20312–20315. [DOI] [PubMed] [Google Scholar]
- 28. Huang C.-J., Zheng Y.-Y., Langmuir 2019, 35, 1662–1671. [DOI] [PubMed] [Google Scholar]
- 29. Muresan N. M., Willkomm J., Mersch D., Vaynzof Y., Reisner E., Angew. Chem. Int. Ed. 2012, 51, 12749–12753; [DOI] [PubMed] [Google Scholar]; Angew. Chem. 2012, 124, 12921–12925. [Google Scholar]
- 30. Materna K. L., Rudshteyn B., Brennan B. J., Kane M. H., Bloomfield A. J., Huang D. L., Shopov D. Y., Batista V. S., Crabtree R. H., Brudvig G. W., ACS Catal. 2016, 6, 5371–5377. [Google Scholar]
- 31. Louette P., Bodino F., Pireaux J.-J., Surf. Sci. Spectra 2005, 12, 133–138. [Google Scholar]
- 32. Bard A. J., Faulkner L. R., Electrochemical Methods: Fundamentals and Applications, Wiley, New York, 2001. [Google Scholar]
- 33. Loftus A. F., Reighard K. P., Kapourales S. A., Leopold M. C., J. Am. Chem. Soc. 2008, 130, 1649–1661. [DOI] [PubMed] [Google Scholar]
- 34. Zhao J., Zhu X., Li T., Li G., Analyst 2008, 133, 1242–1245. [DOI] [PubMed] [Google Scholar]
- 35. Laviron E., J. Electroanal. Chem. 1979, 101, 19–28. [Google Scholar]
- 36. Hanna C. M., Sanborn C. D., Ardo S., Yang J. Y., ACS Appl. Mater. Interfaces 2018, 10, 13211–13217. [DOI] [PubMed] [Google Scholar]
- 37. Abdiaziz K., Salvadori E., Sokol K. P., Reisner E., Roessler M. M., Chem. Commun. 2019, 55, 8840–8843. [DOI] [PubMed] [Google Scholar]
- 38. Haugland M. M., Anderson E. A., Lovett J. E., in Electron Paramagnetic Resonance 2017, pp. 1–34. [Google Scholar]
- 39. Tansakul C., Lilie E., Walter E. D., Rivera F., Wolcott A., Zhang J. Z., Millhauser G. L., Braslau R., J. Phys. Chem. C 2010, 114, 7793–7805. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 40. Hickey D. P., Milton R. D., Chen D., Sigman M. S., Minteer S. D., ACS Catal. 2015, 5, 5519–5524. [Google Scholar]
- 41. Das A., Stahl S. S., Angew. Chem. Int. Ed. 2017, 56, 8892–8897; [DOI] [PMC free article] [PubMed] [Google Scholar]; Angew. Chem. 2017, 129, 9018–9023. [Google Scholar]
- 42. Bailey W. F., Bobbitt J. M., Wiberg K. B., J. Org. Chem. 2007, 72, 4504–4509. [DOI] [PubMed] [Google Scholar]
- 43. Rafiee M., Miles K. C., Stahl S. S., J. Am. Chem. Soc. 2015, 137, 14751–14757. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 44. Wu X., Fan X., Xie S., Lin J., Cheng J., Zhang Q., Chen L., Wang Y., Nat. Catal. 2018, 1, 772–780. [Google Scholar]
- 45. Costentin C., Drouet S., Robert M., Savéant J. M., J. Am. Chem. Soc. 2012, 134, 11235–11242. [DOI] [PubMed] [Google Scholar]
- 46. Dalle K. E., Warnan J., Leung J. J., Reuillard B., Karmel I. S., Reisner E., Chem. Rev. 2019, 119, 2752–2875. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 47. Zhang X., Wu Z., Zhang X., Li L., Li Y., Xu H., Li X., Yu X., Zhang Z., Liang Y., Wang H., Nat. Commun. 2017, 8, 14675. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 48. Wang M., Torbensen K., Salvatore D., Ren S., Joulié D., Dumoulin F., Mendoza D., Lassalle-Kaiser B., Işci U., Berlinguette C. P., Robert M., Nat. Commun. 2019, 10, 3602. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 49. Liu Y., McCrory C. C. L., Nat. Commun. 2019, 10, 1683. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 50. Roy S., Reisner E., Angew. Chem. Int. Ed. 2019, 58, 12180–12184; [DOI] [PMC free article] [PubMed] [Google Scholar]; Angew. Chem. 2019, 131, 12308–12312. [Google Scholar]
- 51. Standard Potentials in Aqueous Solution (Eds.: A. J. Bard, R. Parsons, J. Jordan), CRC, New York, 1985. [Google Scholar]
- 52. Nutting J. E., Rafiee M., Stahl S. S., Chem. Rev. 2018, 118, 4834–4885. [DOI] [PMC free article] [PubMed] [Google Scholar]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.