Abstract
Electrolyzers are now capable of reducing carbon dioxide (CO2) into products at high reaction rates but are often characterized by low energy efficiencies and low CO2 utilization efficiencies. We report here an electrolyzer that reduces 3.0 M KHCO3(aq) into CO(g) at a high rate (partial current density for CO of 220 mA cm–2) and a CO2 utilization efficiency of 40%, at a voltage of merely 2.3 V. These results were made possible by using: (i) a reactive carbon solution enriched in KHCO3 as the feedstock instead of gaseous CO2; (ii) a cation exchange membrane instead of an anion exchange membrane, which is common to the field; and (iii) the hydrogen oxidation reaction (HOR) at the anode instead of the oxygen evolution reaction (OER). The voltage reported here is the lowest reported for any CO2 to CO electrolyzer that operates at high current densities (i.e., a partial current density for CO greater than 200 mA cm–2) with a CO2 utilization efficiency of greater than 20%. This study highlights how the choice of feedstock, membrane, and anode chemistries affects the rate and efficiency at which CO2 is converted into products.
Short abstract
The electrolytic reduction of reactive carbon solutions into carbon-containing products can be achieved at a high rate of production with high energy efficiency and carbon yield.
The CO2 reduction reaction (CO2RR) is a means of using electricity to convert CO2 into fuels and chemicals.1−4 A commercial CO2RR electrolyzer will likely need to operate at current densities (j) greater than 200 mA cm–2 and cell voltages (Vcell) below 3 V.5−9 The only laboratory-scale CO2RR electrolyzers that meet these criteria use anion exchange membranes (AEMs) to separate the cathode and anode compartments.9−12 The AEM creates an alkaline environment at the cathode and anode electrodes.13 The alkalinity at the anode reduces the applied potential required to drive the oxygen evolution reaction (OER) and enables the use of inexpensive nickel electrodes.14 However, the alkalinity at the cathode also converts the CO2 reactant into (bi)carbonates (eq 1).15,16 This situation is problematic because (bi)carbonates are electrochemically inert and can migrate across the AEM to react with H+ in the anode chamber to regenerate CO2.9,14 Consequently, the maximum possible CO2 utilization efficiency (eq 2) for CO production is 50% for a CO2RR electrolyzer that does not neutralize the OH– byproduct (Figure 1); that is, one molecule of CO is produced for every two molecules of CO2 entering the electrolyzer at steady state.17 In practice, CO2 utilization efficiencies of <20% are generally observed for CO2RR electrolyzers that contain an AEM to separate the OER and CO2RR in the anode and cathode chambers, respectively (denoted “OER|AEM|CO2” to indicate the anode|membrane|cathode configuration).18 Moreover, the O2 produced at the anode of OER|AEM|CO2 electrolyzers has little economic value and is therefore not utilized.14
1 |
2 |
CO2RR electrolyzers that use bipolar membranes (BPMs) instead of AEMs convert a larger fraction of the CO2 feedstock into CO (Figure 1).20−22 BPMs dissociate water at the interface of an AEM and a CEM to deliver OH– and H+ to the anode and cathode, respectively (eq 3). The H+ supplied to the cathode reacts with bicarbonate to form CO2in situ (eq 4). The H+ also neutralizes the OH– product formed during CO2RR electrolysis (eq 5), which negates the alkalinity problem encountered with AEMs.23 However, at high current densities a significant potential is required to dissociate water into H+ and OH– using a BPM.24 This potential can be reduced using a water dissociation catalyst.25 However, CO2RR electrolyzers that use BPMs currently require much more than 3 V to realize jCO >200 mA cm–2 (Figure 1).14 It is for these reasons that neither a BPM or an AEM electrolyzer has simultaneously demonstrated high CO2 utilizations and low voltages (Figure 1).20,26−29
3 |
4 |
5 |
Another factor to consider is where the gaseous CO2 feedstock is derived from. This feedstock requires the isolation, purification, and compression of CO2 before it enters a CO2RR electrolyzer.30,31 The isolation of CO2 from air capture streams requires 23 MJ to convert 100 mol of K2CO3 into CO2,30 and CO2 compression requires 2 MJ per 100 mol of CO2.32 These steps are capital intensive, and the energy penalties are significant relative to electrolysis (12 MJ per 100 mol CO2; Table S1). Moreover, the low CO2 utilization efficiencies obtained with OER|AEM|CO2 electrolyzers increase the cost of separating unreacted CO2 from the product stream.33
We report here a “bicarbonate electrolyzer” that solves the aforementioned problems by (i) reducing “reactive carbon solutions” (instead of gaseous CO2) into CO at the cathode, (ii) replacing the AEM with a CEM, and (iii) replacing the OER with the HOR at the anode. Reactive carbon solutions are defined herein as the aqueous eluent from carbon capture units that use hydroxide to capture CO2. These bicarbonate-enriched solutions enable captured carbon to be delivered to the electrolyzer as a liquid (e.g., KHCO3(aq)) rather than as gaseous CO2. This liquid feed not only simplifies the design of the electrolyzer, but also helps to increase CO2 utilization efficiency and bypasses the need to thermally generate pure CO2 upstream of the electrolyzer.26 The CEM also lowers Ohmic resistances relative to an AEM by transporting highly mobile H+ (ionic mobility 36 × 10–8 m2 s–1 V–1) instead of OH– (ionic mobility 21 × 10–8 m2 s–1 V–1; note that CO32– is actually the dominant charge carrier in current AEM CO2RR electrolyzers and is characterized by an even lower ionic mobility of 7.5 × 10–8 m2 s–1 V–1).13,15,34 Moreover, CEMs avoid the high water dissociation overpotential associated with BPMs. The transport of H+ by the CEM into the cathode compartment enables the conversion of bicarbonate into electrochemically active CO2 at the cathode (eq 4). The oxidation of hydrogen gas instead of water at the anode also serves to lower the applied potential required to drive electrolysis. These collective features of our electrolyzer (denoted “HOR|CEM|HCO3–” to reflect the configuration) enabled a partial current density for CO of 220 mA cm–2 at a cell voltage of 2.3 ± 0.1 V and a CO2 utilization efficiency of 40 ± 2%. The lowest previously reported voltage for a CO2RR electrolyzer that operates at a partial current density for CO >200 mA cm–2 is 2.8 V and 16% CO2 utilization.35
Results and Discussion
The HOR|CEM|HCO3– electrolyzer reported here presses the anode and cathode tightly against opposite faces of Nafion, a CEM (Figure 1). Flowplates with serpentine channels were used to deliver humidified H2 gas and 3 M KHCO3 to the anode and cathode, respectively. The gas diffusion electrode (GDE) in the anode chamber consisted of platinum on carbon black, while a silver-foam electrode was used in the cathode chamber. This electrolyzer was used to perform electrolysis experiments at applied current densities over a 100–1000 mA cm–2 range. Product formation rates of CO and H2 from the cathode compartment along with Vcell values (the cell voltage measured across the anode and cathode) were recorded over the course of the electrolysis experiments. Measurements of the unreacted H2 from the anode showed H2 utilization values of up to 28% (Figure S2). The electrolysis experiments were performed under different pressures using a custom-made pressurized electrolyzer test station (Figure S3).19
Electrolysis experiments using this reactor architecture at an applied current density of 100 mA cm–2 and ambient conditions yielded a Vcell value of 1.7 ± 0.1 V (Figure 2). This value represents the lowest Vcell value ever reported for a liquid-fed CO2RR electrolyzer. When the current density was held at 500 mA cm–2, the Vcell value was measured to be 2.3 ± 0.1 V, setting a new benchmark for CO2 electrolysis.
We plotted Vcell values over a range of current densities against those obtained with our previously reported bicarbonate electrolyzer OER|BPM|HCO3– (Figure 2). The OER|BPM|HCO3– electrolyzer contains a BPM (instead of Nafion) and mediates the OER at a nickel anode (instead of the HOR at a platinum anode). In order to maintain a current density of 100 mA cm–2, OER|BPM|HCO3– required a Vcell value of 4.0 ± 0.3 V. This value is more than twice as high as that for HOR|CEM|HCO3–, which performs the HOR at the anode. The Vcell value of OER|BPM|HCO3– spiked to 12.7 ± 3.3 V at 500 mA cm–2, whereas the Vcell value of HOR|CEM|HCO3– was only 2.3 ± 0.1 V at this current density (Figure 2). The low measured voltage of HOR|CEM|HCO3– relative to OER|BPM|HCO3– is due not only to the lower thermodynamic voltage limit (achieved by substituting the OER for the HOR), but also the lower overpotentials of the HOR in comparison to the OER and water dissociation reaction (Figure S4).5,36 The thinner CEM also reduces Ohmic resistances relative to the BPM (the CEM is 25 or 50 μm, whereas the BPM is 195 μm).37,38 The voltage penalties for water dissociation and the OER render the Vcell value for the OER|BPM|HCO3– electrolyzer impractical.
While the Vcell values for HOR|CEM|HCO3– are state of the art, the measured Faradaic efficiencies for CO production (FECO) were merely 40 ± 3% at 100 mA cm–2 (15 ± 3% at 500 mA cm–2; Figure 2). A supply of H+ from the membrane to the cathode is required for in situ CO2 (i-CO2) generation (eq 4); however, this H+ flux can contribute to the parasitic hydrogen evolution reaction (HER). We therefore added a buffer layer between the cathode and membrane to mitigate the HER by managing H+ transport to the cathode.39 This buffer layer increased the FECO value from 40% to 71% at 100 mA cm–2 (Figure S5).
We increased the FECO values even further by pressurizing the bicarbonate feedstock, which increases the CO2 solubility.19 The pressurized HOR|CEM|HCO3– electrolyzer under 3.5 atm of pressure yielded a FECO value of 89 ± 11% at 100 mA cm–2 and 44 ± 1% at 500 mA cm–2 (Figure 2). The molar composition of the gaseous cathode outlet stream at 500 mA cm–2 was 30% CO2(g), 22% CO(g), and 48% H2(g). The HOR|CEM|HCO3– electrolyzer therefore achieved a jCO value of ∼220 mA cm–2, the highest value reported for CO2RR electrolyzers using a liquid feedstock (Figures S6 and S7). Importantly, the CO2 utilization value was measured to be 40 ± 2%, which is higher than that for any OER|AEM|CO2 electrolyzer which achieves jCO > 200 mA cm–2.18 The cell voltage was stable for 10 h. The slight decrease in FECO values could be caused by degradation of the platinum anode catalyst over time (Figure S8).40
The HOR|CEM|HCO3– electrolyzer uses (i) a reactive carbon solution feedstock to bypass CO2 desorption upstream of the electrolyzer and (ii) the HOR at the anode to eliminate the OER voltage penalty. However, the OER|AEM|CO2 electrolyzer achieves a higher FECO in comparison to the HOR|CEM|HCO3– electrolyzer, and it does not require H2 gas. We therefore performed a mass and energy balance to compare these two types of electrolyzer architectures. This analysis encompasses the energy required for the capture, regeneration, and electrolysis of 100 mol of CO2. Importantly, the analysis accounts for the CO2 utilization efficiency of each electrolyzer. The Sankey diagram in Figure 3 illustrates how a HOR|CEM|HCO3– electrolyzer with a CO2 utilization efficiency of 40% yields CO with a higher energy efficiency (1.4 MJ mol–1 CO) in comparison to a OER|AEM|CO2 electrolyzer (1.9 MJ mol–1 CO) operating at a CO2 utilization efficiency of 20%.17 Another advantage of bicarbonate electrolysis is that it does not require the high temperatures and pressures used for thermochemical CO2 hydrogenation.41
While the Sankey diagram shows that the HOR|CEM|HCO3– consumes less energy than the OER|AEM|CO2 electrolyzer, it requires H2 gas to be fed to the anode. This reaction reduces electricity consumption relative to the OER, but the source and cost of H2 must be considered. Ideally, H2 would be produced from a low-carbon source such as biomass gasification or water electrolysis.44 The cost of generating H2 by biomass gasification is reported to be as low as $0.9/kg45,46 (with net negative emissions of 15–22 kg CO2/kg H2 when it is coupled to carbon capture and sequestration47,48), and the target price for clean H2 determined by the DOE Energy Earthshots Initiative is $1 per kg of H2.49 We therefore used a forward-looking purchase price of $1/kg of H2 as a basis for comparing the economics of HOR|CEM|HCO3–, which consumes H2, to the OER|BPM|HCO3– and conventional OER|AEM|CO2, which consume water at the anode (Table 1 and Figure S9). We adopted widely used assumptions for future market conditions for this analysis (electricity $0.03/kWh, $50/tonne CO2, CO sale price of $0.60/kg)7 and electrolyzer performance specifications (voltages, Faradaic efficiencies, CO2 utilization efficiencies) for each of the three electrolyzer technologies (Figure S9). We assumed FECO values of 100% for the OER|AEM|CO2 and 80% for the HOR|CEM|HCO3– and OER|BPM|HCO3– electrolyzers, assumed a current density of 500 mA cm–2, and expressed the voltages as slightly better than current state of the art metrics for the three electrolyzer technologies (Table 1). To determine the CO2 capture and separation costs, we used CO2 utilization efficiencies of 20% for the OER|AEM|CO2 and 40% for the HOR|CEM|HCO3– and OER|BPM|HCO3– electrolyzers.
Table 1. Input and Output Parameters from the Technoeconomic Analysis of Three Electrolyzers.
HOR|CEM|HCO3– | OER|BPM|HCO3– | OER|AEM|CO2 | |
---|---|---|---|
Input Parameters | |||
voltage (V) | 2 | 4 | 3 |
CO2 utilization (%) | 80 | 80 | 40 |
FECO (%) | 80 | 80 | 100 |
j (mA cm–2) | 500 | ||
gross cost of CO2 capture ($/ton) | 50 | ||
installed capex cost ($/kW) | 450 | ||
electricity ($/kWh) | 0.03 | ||
H2 purchase price ($/kg) | 1 | N/A | N/A |
Output Parameters | |||
cost of H2 ($M/yr) | 2.61 | 0.00 | 0.00 |
electricity cost ($M/yr) | 5.24 | 10.48 | 6.29 |
CO2 capture cost ($M/yr) | 1.06 | 1.06 | 2.87 |
CO2 separation cost ($M/yr) | 0.72 | 0.72 | 4.30 |
maintenance and water cost ($M/yr) | 0.25 | 0.49 | 0.3 |
total opex ($M/yr) | 9.88 | 12.75 | 13.75 |
total capex: electrolyzer + balance of plant ($M) | 13.8 | 27.6 | 16.56 |
Revenue from Sale of CO at $0.60/kg ($M/yr) | 21.90 | ||
profit | 11.52 | 8.78 | 7.82 |
NPV 20 yearsa | 48.96 | 23.7 | 28.08 |
The net present value (NPV) was calculated on the basis of a 20 year plant life, 10% interest rate, 38.9% income tax rate, 2.5% fixed operating cost, and a depreciation schedule based on the modified accelerated cost recovery system that was developed by the Department of Energy for water electrolyzer and hydrogen technologies.
The outcome of this technoeconomic analysis is that the HOR|CEM|HCO3– electrolyzer is the most profitable option of the three electrolyzers (see NPV values in Table 1). The primary drivers for the profitability of a bicarbonate electrolyzer coupled to a H2 production plant are: (i) the lower electricity costs due to the lower operating voltage; (ii) the lower CO2 capture and separation costs due to the elimination of CO2 regeneration; and (iii) the higher CO2 utilization efficiencies. We note that the recycling of H2 can further minimize costs. For example, the proof of concept experiments in Figure S10 demonstrate that the amount of virgin H2 supplied to the system can be reduced by recycling H2 during the production of formate at the cathode. Formate was targeted for this experiment because CO poisons platinum catalysts used for the HOR and would therefore need to be separated before recycling.50
We demonstrate here an electrolyzer that mediates the conversion of reactive carbon solutions enriched with bicarbonate into CO with a partial current density of 220 mA cm–2 at merely 2.3 V. This high CO formation rate and low voltage set a benchmark for reactive carbon capture. The CO2 utilization value of 40% is also state of the art at high current densities (i.e., 500 mA cm–2). By sourcing H+ from the HOR instead of the OER, the HOR|CEM|HCO3– electrolyzer requires 2.3 V to drive bicarbonate electrolysis at 500 mA cm–2 instead of 12.7 V for OER|BPM|HCO3–. Moreover, we show that the FECO value of the electrolyzer can be increased to 89% at 100 mA cm–2 and 44% at 500 mA cm–2 by pressurizing the electrolyzer to increase CO2 solubility. With these performance parameters, our technoeconomic analysis (TEA) shows that coupling the HOR with bicarbonate electrolysis can generate CO more profitably than a traditional OER|AEM|CO2 electrolyzer. These findings demonstrate a practical method for producing value-added carbon products from reactive carbon capture with low electrical energy input.
Methods
KHCO3 (99.5%, Alfa Aesar, USA), 50 wt % platinum on Vulcan XC 72 nanopowder (PK catalyst), and ethylenediaminetetraacetic acid (EDTA; 99%, Sigma-Aldrich, USA) were purchased and used as received. Carbon cloth gas diffusion layers (GDLs; Sigracet 39BB), Fumasep FBM bipolar membranes (BPMs), and Nafion PFSA NR-211 and 212 were purchased from Fuel Cell Store (USA). The BPMs were stored in 1 M NaCl, and the Nafion membranes were stored in 1 M KOH prior to use. Silver foams were obtained from Jiangsu Green Materials Hi-Tech. Co. Ltd. (China). Nafion 117 solutions (5 wt %; in a mixture of lower aliphatic alcohols and water) were obtained from Sigma-Aldrich, USA.
A CH instrument 660D potentiostat (USA) equipped with an Amp booster, and Keithley Precision Measurment DC Supply were used for electrolysis experiments. An Ag/AgCl (3 M NaCl) reference electrode (BASi) was used for cathode potential measurements. A gas chromatography instrument (GC; PerkinElmer, Clarus 580), equipped with a packed MolSieve 5 Å column and a packed HayeSepD column, was used to detect CO and H2 using a flame ionization detector (FID) and a thermal conductivity detector (TCD), respectively. The concentrations of the products CO and H2 (ppm) in the headspace of the catholyte reservoir were quantified by calibrating the signal area for CO and H2 to known concentrations of the two gases.
Electrode Preparation
The silver foam was cut into the desired dimensions (2 × 2 cm) with a blade and washed with acetone and water. The silver foam was treated with dilute nitric acid solution (30% v/v HNO3) in a 50 mL beaker for 10 s to remove the oxide layer and increase its electrochemical surface area. The etched silver foam was then washed thoroughly with deionized (DI) water and 3 M KHCO3 prior to use.
To fabricate the Pt/C gas diffusion electrode (GDE), 8 mg of Pt/C was added to a 2.5 mL mixture of water and isopropanol (IPA) solution (VH2O:VIPA = 4:1) with 20 wt % Nafion solution (5 wt %). The ink was sonicated in a bath sonicator for 15 min and then drop-casted onto a GDL. The fabricated GDEs were then stored in a fume hood to dry overnight.
Electrolysis
A peristaltic pump was used to deliver 1.0 M KOH to the anode of the control system at a constant flow rate of 40 mL min–1. High-purity H2 (10–200 sccm, 99.999%) was humidified in a bubbler held at a constant temperature of 60 °C prior to being fed to the anode of HOR|CEM|HCO3– (Figure S5). Two 127 μm polytetrafluoroethylene (PTFE) gaskets were placed separately between the anode and anodic flowplate and the cathode and cathodic flowplate to prevent leakage for all of the electrolyzers. The catholyte (3.0 M KHCO3) was delivered at a constant flow rate of 100 mL min–1 for all electrolyzers. Gaseous products (e.g., H2 and CO) in the headspace of the cathode electrolyte reservoir were delivered to an in-line gas chromatograph (GC) by a constant rate of N2 flow at 175 sccm for quantification at 350 s. The actual flow rate of the gas mixture was measured by a flow meter positioned immediately downstream of the GC. Liquid products collected from the catholyte after 1200 s of electrolysis were quantified by 1H NMR spectroscopy using potassium hydrogen phthalate as the internal standard with a calibration curve.
Safety Statement
No unexpected or unusually high safety hazards were encountered.
Acknowledgments
The authors are grateful to Dr. Roxanna Delima and Dr. Yong Wook Kim for their valuable suggestions and discussions. The authors are grateful to Natural Resources Canada (EIP2-MAT-001), the Canadian Natural Science and Engineering Research Council (CRDPJ 536621-18), the Canadian Foundation for Innovation (229288), the Canadian Institute for Advanced Research (BSE-BERL-162173), TOTAL American Services, Inc. (an affiliate of TotalEnergies SE, France), and the Canada Research Chairs for financial support. This research was undertaken thanks in part to funding from the Canada First Research Excellence Fund, Quantum Materials and Future Technologies Program. Supplementary data sets generated in the current study are available from the corresponding author upon reasonable request.
Supporting Information Available
The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acscentsci.2c00329.
Faradaic efficiency calculation, liquid product detection, CO2 utilization calculation, pressurized electrolyzer test station, technoeconomic analysis, energy consumption analysis (Sankey diagram), diagram of the experimental setup, the effect of the H2 flow rate on the cell voltage and FECO, membrane thickness effect, Vcell–jCO relationship, stability test, and H2 recycling data (PDF)
Author Contributions
⊥ Z.Z. and E.W.L. contributed equally to this work.
Author Contributions
C.P.B. supervised the project. Z.Z. and C.P.B. conceived the study, and Z.Z. performed the experiments. E.W.L. designed the pressurized system, performed the technoeconomic analysis, and determined the mass and energy balances. S.R. performed experiments and an analysis and aided in technical editing. B.A.W.M. performed an analysis and aided in writing and technical editing. A.H. contributed to an analysis of experimental data. C.P.B., Z.Z., and E.W.L. wrote the first draft of the manuscript. All authors contributed to the writing of the final manuscript.
The authors declare the following competing financial interest(s): The authors C.P.B. and Z.Z. have filed a patent related to this work (No. PCT/CA2022/050094; US patent application No. 63/140.167).
Supplementary Material
References
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