Literature DB >> 36148000

Harvesting Electrical Power during Carbon Capture using Various Amine Solvents.

Trevor J Kalkus1, Caitlin J Shanahan1, Jansie Smart2, Ali Coskun2, Michael Mayer1.   

Abstract

There exists an urgent demand for the advancement of technologies that reduce and capture carbon dioxide (CO2) emissions to mitigate anthropogenic contributions to climate change. This paper compares the maximum power densities achieved from the combination of reverse electrodialysis (RED) with carbon capture (CC) using various CC solvents. Carbon capture reverse electrodialysis (CCRED) harvests energy from the salinity gradients generated from the reaction of CO2 with specific solvents, generally amines. To eliminate the requirement of freshwater as an external resource, we took advantage of a semiclosed system that would allow the inputs to be industrial emissions and heat and the outputs to be electrical power, clean emissions, and captured CO2. We assessed the power density that can be attained using CCRED with five commonly studied CC solvents: monoethanolamine (MEA), diethanolamine (DEA), N-methyldiethanolamine (MDEA), 2-amino-2-methyl-2-propanol (AMP), and ammonia. We achieved the highest power density, 0.94 W m-2 cell-1, using ammonia. This work provides a foundation for future iterations of CCRED that may help to incentivize adoption of CC technology.
© 2022 The Authors. Published by American Chemical Society.

Entities:  

Year:  2022        PMID: 36148000      PMCID: PMC9483915          DOI: 10.1021/acs.energyfuels.2c02279

Source DB:  PubMed          Journal:  Energy Fuels        ISSN: 0887-0624            Impact factor:   4.654


Introduction

Anthropogenic emissions of carbon dioxide (CO2) and other greenhouse gases contribute significantly to climate change, influencing many environmental and biological phenomena, including, but not limited to, extreme weather patterns and ocean acidification.[1,2] A large variety of sustainable technologies have been introduced to reduce the dependence on the combustion of fossil fuels.[1] These efforts include green energy technologies that harvest electrical power from solar power, wind power, geothermal heat, and other renewable resources.[3] Although these technologies have been improving rapidly, they are still insufficient to address the current crisis, especially as energy demands continue to rise.[4] Another category of sustainable energy involves harvesting energy from salinity gradients and has been labeled ‘blue energy’.[5,6] Reverse electrodialysis (RED) and pressure retarded osmosis (PRO) are the most common implementations of blue energy.[5,6] The process of PRO uses a semipermeable membrane to separate two solutions with different salinities. As water migrates to the higher salinity solution, the resulting pressure is used to generate electrical power in a turbine.[7−9] The greatest limitation of PRO is the development of supported semipermeable membranes with high permeability to water.[10,11] When harvesting energy from the mixing of freshwater and seawater, RED achieves higher power density and higher energy recovery than PRO, and improvements to RED systems have been more successful than improvements to PRO.[10−12] The process of RED uses charge-selective membranes to separate a high-salinity solution (traditionally seawater) and a low-salinity solution (traditionally freshwater).[13−15] As ions from the high-salinity solution diffuse to the low-salinity solution, charge selective membranes restrict the diffusion of cations to one direction and the diffusion of anions to the opposite direction (Figure a).[13−15] The resulting separation of charges creates a potential difference across each charge-selective membrane, and the sum of these potentials in series results in the total potential difference across the entire device.[13−15] Although a significant amount of energy can theoretically be made available while large volumes of freshwater and saltwater mix,[16] access to this process is limited to specific geographic areas.[17] The use of concentrated brines from some industrial activities can also provide a source of high-salinity solutions and can even increase the power that can be produced using RED.[18] The development of RED, however, has not yet resulted in a cost-efficient method for providing renewable energy.[15,17,19] A significant reason RED falls short of expectations is the fouling that occurs on the charge-selective membranes when using natural solutions.[20,21] In pilot-scale tests of RED, artificial solutions provided nearly double the power density compared to natural solutions with the same conductivity.[22]
Figure 1

Illustration depicting the concept of combining carbon capture (CC) and reverse electrodialysis (RED). (a) Depiction of RED. Solutions of low- and high-salinity flow past each other separated only by charge-selective membranes in a repeating pattern: high-salinity solution (red), cation-selective membrane (green), low-salinity solution (blue), and anion-selective membrane (yellow). The controlled diffusion of ions leads to a separation of charges, generating a potential difference across each charge selective membrane. This potential difference can be harvested in the form of electrical power. (b) Depiction of solvent-based CC. The CO2 in industrial emissions reacts with the CC solvent in the absorber, generating the rich solution. After CO2 removal, only clean emissions are released, and the CO2-rich solution is delivered to the stripper. In the stripping process, the rich solution is heated to release CO2 gas, which is then sequestered or utilized, resulting in the regeneration of the lean solution, which is delivered back to the absorber. To conserve energy, the solutions pass through a heat exchanger as they circulated so that the heated lean solution will transfer heat to the rich solution before entering the stripper. (c) By using the lean and rich solutions as the low- and high-salinity solutions for RED, the infrastructure already established for heat exchange during the CC process theoretically provides the conditions for the implementation of CCRED, which similarly requires the regular circulation of both solutions in close contact.

Illustration depicting the concept of combining carbon capture (CC) and reverse electrodialysis (RED). (a) Depiction of RED. Solutions of low- and high-salinity flow past each other separated only by charge-selective membranes in a repeating pattern: high-salinity solution (red), cation-selective membrane (green), low-salinity solution (blue), and anion-selective membrane (yellow). The controlled diffusion of ions leads to a separation of charges, generating a potential difference across each charge selective membrane. This potential difference can be harvested in the form of electrical power. (b) Depiction of solvent-based CC. The CO2 in industrial emissions reacts with the CC solvent in the absorber, generating the rich solution. After CO2 removal, only clean emissions are released, and the CO2-rich solution is delivered to the stripper. In the stripping process, the rich solution is heated to release CO2 gas, which is then sequestered or utilized, resulting in the regeneration of the lean solution, which is delivered back to the absorber. To conserve energy, the solutions pass through a heat exchanger as they circulated so that the heated lean solution will transfer heat to the rich solution before entering the stripper. (c) By using the lean and rich solutions as the low- and high-salinity solutions for RED, the infrastructure already established for heat exchange during the CC process theoretically provides the conditions for the implementation of CCRED, which similarly requires the regular circulation of both solutions in close contact. The development and adoption of sustainable technologies has been insufficient to meet the goals for the reduction of carbon emissions.[4,23] For these reasons, many scientists, nations, and industries expect that carbon capture (CC) technology will be essential for effectively reducing atmospheric concentrations of greenhouse gases.[24−26] One of the most developed and studied methods for CC is chemisorption, which often involves the use of an amine solvent that reacts with the CO2 (Figure b).[25,27,27−29] The solvent solution that contains little to no CO2 is referred to as a CO2-lean solution (henceforth a lean solution), and the solvent solution that has reacted with and absorbed CO2 is referred to as a CO2-rich solution (henceforth a rich solution). To regenerate the lean solution after it has been loaded with CO2, the rich solution is heated to recover the CO2 via the stripping process.[25,27] The pure CO2 is then stored or utilized, and the CC solution can be reused.[24,30,31] The energetic cost of this solvent regeneration, however, is a primary reason that CC technology is not more widely adopted.[27,28,32−34] For example, the energy necessary to regenerate solvent when this method is used to clean emissions from a coal-burning power plant can increase the energy requirements of the plant by 25–40%.[35] The energetic cost, and the corresponding monetary cost, disincentivizes the implementation of CC technology.[35] To conserve energy, implementations of solvent-based CC use a heat exchanger between the CO2 absorption process, which generally benefits from a low-temperature solution, and the CO2 stripping process, which requires high temperatures (Figure b).[28] The energetic costs of CC may also be reduced by using CC solvents that require less energy to be regenerated.[27,28,32,35] To generate value from carbon utilization to motivate CC, large amounts of capital have been invested into accelerating technologies that utilize CO2.[36,37] Kim et al. recently suggested that value can be created during the CC process by harvesting electric power using RED.[23] They demonstrated the integration of CC and RED, an approach labeled carbon capture reverse electrodialysis (CCRED), and suggested that this combination can address shortcomings of both individual processes.[23] Because the amine solutions that are used for CCRED are not collected from natural sources, membrane fouling may be less likely than when using freshwater and seawater.[20] Additionally, the electrical power generated by RED can be used to help reduce the energetic costs of CC.[23] Although CCRED is unlikely to address all of the energy requirements of CC, the reduced cost can contribute to increasing the economic motivation for implementing CC technology. The reaction of CO2 with an amine CC solvent generates ionic species (eqs –5). This increase in salinity allows for the rich solution to be used as a high-salinity solution for RED.[23] Kim et al. used distilled water as the low-salinity solution for their CCRED device.[23] Distilled water is an external resource that would be required in continuous supply, and it would become polluted with the CC solvent during the CCRED process, requiring additional precautions for disposal in an environmentally safe way. By using distilled water as the low-salinity solution, the CCRED design proposed by Kim et al. would likely not be practical for implementation in full-scale CC systems.[23] Recently, we demonstrated that lean CC solutions can be used as the low-salinity solution instead of distilled water.[38] In principle, this design allows the amine solutions to remain in a closed system with flue gas and heat as inputs and pure CO2, treated emissions, and electrical energy as outputs. Additionally, because the conductivity of the lean solution is higher than that of distilled water, the use of the lean solution reduces the internal resistance of the device and increases power density.[38] Most significantly, the implementation of CCRED in existing CC infrastructure may be relatively seamless considering that the heat exchanger already provides a step in the process where the lean and rich solutions flow past each other in close contact (Figure c). In this work, we focused on analyzing a feature unique to the combination of CC and RED: the difference in power density that results from using different CC solvents. A variety of CC solvents have been investigated in an attempt to find a best candidate for industrial scale CC.[27,29,32] The benchmark for CC solvents has been monoethanolamine (MEA) due to its rapid reaction kinetics with CO2, ensuring efficient CO2 capture.[27,32,39,40] For this reason, we used MEA in previous work when we demonstrated a novel CCRED design that could produce electrical power from the ion gradient generated when capturing CO2 in breath.[38] In the CCRED device presented by Kim et al., the authors used N-methyldiethanolamine (MDEA) because the energy required to regenerate MDEA is lower than that required for MEA.[23] A number of other CC solvents, including diethanolamine (DEA), 2-amino-2-methyl-2-propanol (AMP), and ammonia, as well as mixes of CC solvents have been proposed to strike the balance between fast reaction kinetics and lowering the regeneration energy cost.[27−29,29,32,33,41−45] Ammonia is a particularly interesting candidate for CCRED because it has already been demonstrated in thermolytic RED systems designed to generate energy from low-grade waste heat.[46−49] Because ammonium bicarbonate will evaporate out of solution as ammonia and CO2 gas at relatively low temperatures (around 60 °C), waste heat from some industrial processes is sufficient to remove these ions.[49] In a completely closed system, an ammonium bicarbonate solution can be used as the high-salinity solution, and low-grade heat can remove the ions to regenerate a low-salinity solution.[49] In principle, the gases and solution could be recycled indefinitely to continuously harvest power from waste heat.[46−49] When using different CC solvents, the reaction with CO2 produces different ionic species; sterically hindered amines become protonated and CO2 forms bicarbonate with water molecules, whereas unhindered amines (MEA and DEA) react directly with CO2 to form carbamates in addition to generating protonated species and bicarbonate (eqs –5).[23,27,45] We have previously demonstrated that the composition of ionic species in salinity gradient power sources impacts the resulting power density.[38,50] Here, we directly compare different CC solvents (MEA, DEA, MDEA, AMP, and ammonia) in the same lab-scale CCRED device and demonstrate that ammonia achieved the highest power density, reaching nearly 1 W m–2 cell–1. Ultimately, these results suggest that CCRED could potentially contribute to economically motivating adoption of CC technology.

Materials and Methods

Materials

All chemicals, monoethanolamine (MEA), diethanolamine (DEA), N-methyldiethanolamine (MDEA), 2-amino-2-methyl-2-propanol (AMP), 32% ammonia solution, potassium carbonate, potassium chloride, potassium hexacyanoferrate (II) and potassium hexacyanoferrate (III), were purchased from Sigma-Aldrich. Silicone rubber sheets (0.5 mm thickness) were ordered from Vibraplast AG. We purchased charge selective membranes, Fumasep FKB-PK-130 (100–130 μm thick, polyether ether ketone (PK) reinforced, cation exchange), FKS-50 (45–55 μm thick, no polymer reinforcement, cation exchange), FAB-PK-130 (100–130 μm thick, PK reinforced, anion exchange), and FAS-50 (45–55 μm thick, no polymer reinforcement, anion exchange) membranes, from Fumatech BWT GmbH. Fumatech specifies that these membranes have a selectivity of 92–99% and are stable within the pH 1–14 range. We made spacers using SEFAR PETEX 07-120/50 mesh (120 μm mesh opening, 50% open area, 80 μm thickness), and some preliminary trials used NITEX 03-170/54 (170 μm mesh opening, 54% open area, 100 μm thickness), from SEFAR AG. We fabricated the electrode compartments from acrylic material at the machine shop at the University of Fribourg, Switzerland. We provided the design modeled in Microsoft 3D builder (Supporting Information, Figure S4). The company SGL Carbon GmbH provided sigracell graphite battery felt, GFD, with 4.6 mm thickness. We purchased platinum wire (0.3 mm diameter) from Alfa Aesar. We purified water to 18.2 MΩ cm with a PURELAB Flex II purifier (ELGA LabWater, Veolia).

Constructing the Electrode Compartments

We soldered a platinum current collecting wire to an electrical pin and glued it using epoxy in the center of each electrode compartment, with the platinum wire inside the compartment and the pin providing access outside the compartment. We embedded the platinum wire in graphite felt that we cut to a circular area of 19.6 cm to fill the electrode compartment. We spread an extremely thin layer of Dow Corning high vacuum grease on the acrylic surface to aid in creating a seal with a silicone layer that served as a gasket for holding a CEM in place to separate the electrode compartment from the neighboring high-salinity compartment. This CEM prevented anions from the electrolyte solution in the electrode compartment from diffusing to other compartments. The electrolyte solution consisted of 0.05 M potassium hexacyanoferrate (II), 0.05 M potassium hexacyanoferrate (III), and 0.5 M potassium chloride. We chose to use the redox reaction of a hexacyanoferrate solution with graphite to convert the ionic current to electric current based on previous assessment of electrode assemblies for RED done by Veerman et al.[51] The standard electrode potential of hexacyanoferrate ([Fe(CN)6]4–/[Fe(CN)6]3–) is E0 = 0.356 V.[51] However, because opposite reactions are occurring at the two electrodes, the Nernst potential of reduction on the cathode is counterbalanced by oxidization on the anode, resulting in a net zero contribution to the overall measured potential.[51] We circulated the electrolyte solution separately through the electrode compartments at the same flow rate as the high-salinity and low-salinity solutions. We used the same electrode setup on both ends of the device.

Constructing the Reverse Electrodialysis Device

The CCRED device was assembled using 0.5 mm thick silicone gaskets, Fumasep FKS-50 as the cation exchange membrane, Fumasep FAS-50 as the anion exchange membrane, and 80 μm thick spacers with 50% open area. The gaskets created a circular effective membrane area of 19.63 cm2 for each membrane. We created the spacers to fit within the gasket so that they occupy each compartment as well as the channels leading to each compartment. We cut the shapes for the silicone gasket material (which formed the low-salinity and high-salinity compartments), the charge-selective membranes, and the spacers using a Cricut Maker cutting machine (Cricut Inc.). The cutting patterns used can be accessed by the link provided in the Supporting Information. Assembling the components proceeded as follows: After the CEM that contained the electrode compartment, a silicone gasket forming a high-salinity compartment was added with a spacer inside the channels and the compartment. We then added an AEM, followed by a silicone gasket forming a low-salinity compartment with a spacer inside the channels and compartment and then a CEM. We repeated this pattern one more time for a total of two cells. We completed the device with the second electrode compartment. We placed the high- and low-salinity gaskets in opposite orientations so that they lead to the appropriate input and output channels (Figure ). Eight bolts, placed through holes on the sides and corners of the device, held the device together tightly and evenly.
Figure 2

Design of the CCRED device. (a) 3D representation of the complete device. The end pieces (gray) contain the graphite felt electrodes (marble pattern) and a platinum wire to collect current. An electrode solution containing potassium hexacyanoferrate (purple arrows) is circulated separately through both terminal compartments at the same rate as the lean and rich solutions circulate through their respective compartments. Cation-exchange membranes (green) separate the electrode compartments. The repeating pattern that composes a single CCRED cell is rich compartment (red), anion-exchange membrane (yellow), lean compartment (blue), and cation-exchange membrane (green). Spacers within the rich and lean compartments are indicated by a mesh texture. The rich solution (red arrow) flows into an inlet at the bottom of one end piece, through the rich compartments, and out an outlet at the top of the other end piece. The lean solution (blue arrow) flows in the opposite direction into an inlet at the bottom of one end piece, through the lean compartments, and out an outlet at the top of the other end piece. Eight holes around the edges of all the compartments allow for bolts that hold the CCRED device together. (b) Pictures of the CCRED device at certain stages as it is being assembled. From left to right: the end piece with a silicone gasket and the graphite felt, the first cation-exchange membrane and rich compartment with spacer, the anion exchange membrane stacked on the previous layer, the lean compartment with spacer, and the final assembly with the second end piece.

Design of the CCRED device. (a) 3D representation of the complete device. The end pieces (gray) contain the graphite felt electrodes (marble pattern) and a platinum wire to collect current. An electrode solution containing potassium hexacyanoferrate (purple arrows) is circulated separately through both terminal compartments at the same rate as the lean and rich solutions circulate through their respective compartments. Cation-exchange membranes (green) separate the electrode compartments. The repeating pattern that composes a single CCRED cell is rich compartment (red), anion-exchange membrane (yellow), lean compartment (blue), and cation-exchange membrane (green). Spacers within the rich and lean compartments are indicated by a mesh texture. The rich solution (red arrow) flows into an inlet at the bottom of one end piece, through the rich compartments, and out an outlet at the top of the other end piece. The lean solution (blue arrow) flows in the opposite direction into an inlet at the bottom of one end piece, through the lean compartments, and out an outlet at the top of the other end piece. Eight holes around the edges of all the compartments allow for bolts that hold the CCRED device together. (b) Pictures of the CCRED device at certain stages as it is being assembled. From left to right: the end piece with a silicone gasket and the graphite felt, the first cation-exchange membrane and rich compartment with spacer, the anion exchange membrane stacked on the previous layer, the lean compartment with spacer, and the final assembly with the second end piece. We implemented a Glison Minipuls 3 peristaltic pump to circulate the solutions through the compartments. We used a flow rate of approximately 7.6 mL min–1 cell–1 for all experiments unless stated otherwise (Supporting Information, Figure S2). For each trial, we first made the lean solution for each solvent at the desired concentration (3.28 M MEA, 3.28 M DEA, 1.74 M MDEA, 1.74 M AMP, 1.74 M ammonia, 3 M ammonia). We then separated half of the lean solution and saturated it with CO2 until the pH stabilized to generate the rich solution. We used four separate channels on the peristaltic pump to simultaneously push the desired lean and rich solution through their respective channels as well as push the electrode solution through each electrode compartment. We used the peristaltic pump to rinse the CCRED device with a 1.74 M KCl solution and a 12 mM KCl solution in the rich and lean compartments, respectively, between uses to remove traces of CC solutions and refresh the membranes.

Characterizing Power

As the rich and lean solutions of the desired solvent traveled through the CCRED device, we measured voltage and current using a Keithley 2400 SourceMeter connected to the electrical pins on the end plates. We allowed for values to stabilize before being recorded (generally around 2 min). We used the measurements of open circuit voltage, voltage with a 99 Ω load, and short circuit current to characterize power density. We normalized power density by cell, which consists of one membrane pair.

Estimating Ammonia Concentration

We found that the aqueous ammonia stock solution (32%) was most likely over the saturation limit at our altitude (610 m) and temperature range. After generating rich solutions of various concentrations, we correlated the measured conductivities with reported conductivities of ammonium bicarbonate in the literature to determine the concentration.[49] Based on the conductivities of the generated solutions, we estimated that the stock solution was approximately 13.77 M ammonia. To limit the loss of ammonia as a gas, all ammonia solutions were kept in sealed containers when not being used, and CO2 was added to the ammonia solution at a slow rate to prevent aggressive bubbling that might allow gas be stripped out of the solution.

Measurements of pH and Conductivity

We measured pH using a calibrated PH8500-SB portable pH meter for strong basic solutions (purchased from Apera Instruments). We measured conductivity using a Seven Compact Duo pH/Conductivity meter from Mettler Toledo.

Addition of CO2

We sourced pure CO2 from a pressurized tank provided by Carbagas AG, and we regulated the pressure to 1 bar. We dispersed CO2 gas into the desired CC solutions using a gas dispersion tube with a porous fritted glass tip, 4–8 μm porosity, produced by Ace Glass, Inc. and purchased from Sigma-Aldrich. A Supelco Rotameter with a needle valve (flow range 0–110 mL min–1) was purchased from Sigma-Aldrich controlled CO2 gas flow rate. We added CO2 until the pH stabilized, indicating maximum carbon loading.

Statistical Analysis

The data are presented as the mean ± standard deviation (SD), with a sample size of n = 3 unless stated otherwise. We propagated uncertainty accordingly when we used measured values in calculations.

Results and Discussion

Design of the Carbon Capture Reverse Electrodialysis Device

When designing a CCRED system, a variety of parameters influence power density (Supporting Information, Figures S1 and S2). For example, reducing the intermembrane distance (the distance that separates the charge-selective membranes) results in a higher power density due to the reduction of internal resistance.[12,52] As the membranes are designed closer together, however, it is more likely that they may bulge and come into contact, especially because of the osmotic pressure caused by the different salinities. To prevent the membranes from touching, mesh spacers are often used in the compartments.[53−56] We modeled the CCRED device in this work after the one presented by Kim et al. (Figure ).[23,57] Kim et al. also demonstrated that open circuit voltage increases as the flow rate of the low- and high-salinity solutions increases because mixing is minimized and the salinity gradient is maintained.[57] We similarly found that faster flow rates resulted in higher open circuit voltage (Supporting Information, Figure S2).

Power Density Generated by Different CC Solvents

In order to compare the performance of different CC solvents, namely, MEA, DEA, MDEA, AMP, and ammonia, using the CCRED device shown in Figure , we sought to generate comparable salinity gradients using each CC solvent because the voltage and power produced by RED relates to the difference in ion concentration between solutions (Supporting Information, Sections S4–S6). The CC solvents react with CO2 differently and have different theoretical maximum carbon loadings. MEA and DEA react to form relatively stable carbamates:[23,27,43,58,59] According to these reactions, it is expected that MEA and DEA (a primary and secondary amine respectively) would be able to capture approximately 0.5 mol of CO2 per mol of amine. Sterically hindered amines and ammonia, on the contrary, do not form stable carbamate species. For this reason, the reaction produces a protonated species and a bicarbonate:[23,29,43−45,60] Using MDEA, AMP, or ammonia, the theoretical carbon loading can reach 1 mol of CO2 per mol of hindered amine or ammonia[23,29,43−45] (Figure shows the chemical structures). We expected twice as many ions to form when capturing CO2 with MDEA, AMP, or ammonia than when using the same concentration of MEA or DEA. We used eqs –5 as guidelines for approximating similar salinity conditions, but we also note that these reactions do not reflect the full complexity of the chemical system in applied settings. For example, in previous work, we captured approximately 0.6 mol of CO2 per mol of MEA.[38] Nonetheless, we expected that these reactions reflected the general relationship of these CC solvents, and, because of the logarithmic relationship between salinity gradient and electric potential (Supporting Information, Equations S1–S4), we considered this approximation to be sufficient for the comparison of the different CC solvents. We generated the rich solution for each CC solution by dispersing CO2 into the solution until the pH stabilized (Table ).
Figure 3

Power characteristics of CCRED using different CC solvents. (a) Maximum power density from CCRED using various CC solvents. The chemical structures of the different CC solvents are shown to the right. (b) Representative current–voltage curve for each CC solvent. A resistive load of 99 Ω was used to acquire the middle datum for each CC solvent. Lines are linear fits. (c) Open circuit voltage and short circuit current of CCRED for each CC solvent.

Table 1

Conductivity of the Lean and Rich Solutions

CC solventsolvent concentration (M)conductivity of lean solution (mS cm–1)pH of lean solutionconductivity of rich solution (mS cm–1)pH of rich solution
MEA3.281.08612.249.707.8
DEA3.280.960311.715.077.9
MDEA1.740.287111.434.697.5
AMP1.740.975612.232.157.9
ammonia1.741.27111.8104.47.9
Power characteristics of CCRED using different CC solvents. (a) Maximum power density from CCRED using various CC solvents. The chemical structures of the different CC solvents are shown to the right. (b) Representative current–voltage curve for each CC solvent. A resistive load of 99 Ω was used to acquire the middle datum for each CC solvent. Lines are linear fits. (c) Open circuit voltage and short circuit current of CCRED for each CC solvent. Figure shows that ammonia produced a higher power density than the other CC solvents. Based on chemical structure, we hypothesized that ammonium cations would migrate across the cation-selective membrane much faster than the bulkier protonated amines generated by the other CC solvents. Having a higher mobility and likely a higher permeability than the other cations, ammonia produced a higher voltage and current than those produced by other CC solvents. We also expected relatively low power output when using MEA and DEA, the solvents that form stable carbamate species, based on the analysis done in previous work that demonstrated that the carbamate formed by MEA had a much lower permeability than bicarbonate across the anion-exchange membrane.[38] We observed that DEA exhibited the highest viscosity and ammonia exhibited the lowest viscosity of the solvents tested, which aligns with DEA producing the lowest short circuit current and ammonia producing the highest short circuit current.

Analyzing Conductivity to Optimize Power Density

The conductivity of the lean and rich solutions influenced the power output by affecting the internal resistance of the device.[38]Table displays the measured conductivities of the different CC solvents at the concentrations used in the experiments presented in Figure . Ammonia had the highest conductivity values among the tested CC solvents for both the rich and the lean solutions. With these measurements, we estimated the resistance from the lean compartments (two compartments in total) and rich compartments (three compartments in total). Using the measured open circuit voltage Voc (V) and short circuit current Isc (A), we solved for the expected total internal resistance Rint (Ω) of the power source for each CC solvent:[61] Figure shows the estimated contribution of the lean and rich compartments as portions of the measured total internal resistance. The charge-selective membranes and electrode compartments likely contributed the remaining resistance.[38] The rich solution contributed a negligible amount of resistance in each case, and optimization of the other components should be prioritized. For example, the resistance contributed by the lean compartment can be decreased by decreasing thickness of the compartment.[12,38] Additionally, Kim et al. and others have advocated for continued research to improve charge-selective membranes, which could also lead to reduced resistance, for example.[23,47,62,63] While the membranes used in this work have been optimized for monatomic salts, like NaCl, it may be possible that membranes specialized for ammonium bicarbonate or the other CC generated ionic species could result in a lower resistance.[23,47,62,63]
Figure 4

Measured internal resistance and the estimated contributions of the rich and lean solutions. The red parts of the bars represent the estimated contribution of the rich solution to the total internal resistance (three compartments). The stacked blue bars represent the estimated contribution of the lean solution to the total internal resistance (two compartments). The membranes and electrodes likely contribute the remaining resistance (black).

Measured internal resistance and the estimated contributions of the rich and lean solutions. The red parts of the bars represent the estimated contribution of the rich solution to the total internal resistance (three compartments). The stacked blue bars represent the estimated contribution of the lean solution to the total internal resistance (two compartments). The membranes and electrodes likely contribute the remaining resistance (black). The contributions to the internal resistance of the CCRED system appeared quite similar for most of the CC solvents with the exception of MDEA. We measured a much lower conductivity of the lean MDEA solution compared to the other CC solvents, but the total Rint of the CCRED device remained similar to the other CC solvents, suggesting that the charge-selective membranes provided much less resistance to MDEA. Kim et al. proposed that, instead of the entire protonated species traveling across the cation-selective membrane, only the proton travels across the membrane.[23] Protons do exhibit exceptional mobility, MDEA has the lowest pKa of the CC solvents we used (Supporting Information, Table S1), and the pH value of the rich MDEA solution was the lowest among all tested solvents (Table ). If the protons traveled across the membrane instead of, or in addition to, the protonated species, their flux may result in a much lower resistance from the cation-selective membrane. The protonation kinetics of MDEA may also account for the low conductivity of the lean MDEA solution. Because of the high contribution of the lean compartment to the overall resistance of the CCRED device, reducing compartment thickness would prove much more beneficial to the power density of CCRED when using MDEA than it would when using the other CC solvents. Ammonia outperformed the other CC solvents in all the aspects important to power density: highest Voc, highest Isc, highest lean solution conductivity, highest rich solution conductivity, and lowest total Rint. Using ammonia, we optimized the concentration based on conductivity to further reduce the internal resistance of the device (Figure ), as demonstrated with MEA in previous work.[38] The highest conductivity measured for ammonia surpassed that of the other CC solvents (Supporting Information, Figure S3).[38]Figure demonstrates that the lean solution contributed much more resistance than the rich solution, so we chose to use the concentration that resulted in the highest conductivity of the lean solution to maximize power density. We measured the highest conductivity of the lean solution at an ammonia concentration of 3 M (Figure ), which agrees with values reported in the literature.[64] At concentrations greater than 3 M ammonia, the enhanced intermolecular association that occurs due to insufficient solvent for complete ion solvation results in decreased conductivity.[64] Using 3 M ammonia, we reached a power density of 0.94 W m–2 (Table ), which is one of the highest power densities reported to date for RED systems using ammonium bicarbonate.[46,48,49,65] This maximum power density also nearly matches the 1 W m–2 achieved by Kim et al.[23] and represents nearly a 10-fold improvement in maximum power density compared to the 0.1 W m–2 achieved by the batch-flow CCRED device presented in previous work.[38]
Figure 5

Conductivity of lean and rich ammonia solutions at different concentrations. (a) Conductivity of lean ammonia solutions at various concentrations. (b) Conductivity of rich ammonia solutions at various concentrations.

Table 2

Conditions for the Highest Open Circuit Voltage, Short Circuit Current, and Maximum Power Density Achieved Using the CCRED Device Presented in This Work

CC solutionpH of lean solutionpH of rich solutionopen circuit voltage (mV cell–1)short circuit current (mA cm–1)maximum power density (W m–2)
3 M ammonia12.17.9250 ± 51.50 ± 0.040.94 ± 0.03
Conductivity of lean and rich ammonia solutions at different concentrations. (a) Conductivity of lean ammonia solutions at various concentrations. (b) Conductivity of rich ammonia solutions at various concentrations.

Energy Analysis

This work focuses on analyzing and optimizing specifically the maximum power density that can be attained by CCRED using different CC solvents. In RED systems, however, a high power density comes at the expense of energy efficiency.[66,67] More energy can be harvested as more ions diffuse across the membrane and more mixing of the two solutions occurs. As mixing occurs, however, the salinity of the two solutions becomes more similar, and the electric potential across the charge-selective membranes decreases, resulting in a corresponding decrease in power density.[66,67] By maximizing power density, we considered time to be the limited resource, and a large amount of energy that could be made available from further mixing was not utilized. If one or both of the lean or rich solutions were a limited resource, it may be advantageous to use large membrane areas and/or slow flow rates to allow for more mixing and to harvest a larger amount of energy per volume of solution. For these reasons, if CCRED were to be implemented on an industrial scale, it would be important to discern the limiting resources and optimize the system accordingly. The theoretical exergy flow rate X (W) of two streams of water with different salinities at the same temperature can be derived from the change in free energy upon the mixing of these streams:[38,46,68]where C is the ionic concentration (M), Q is the flow rate (L s–1), and subscripts indicate the low-salinity solution (LSS), the high-salinity solution (HSS), and the mixed solution (MIX). Using ion activity instead of ion concentration would solve for exergy more accurately, but, because ion activity at such high concentrations of ammonium bicarbonate is unavailable in the literature and is also difficult to estimate,[46,69,70] we approximated exergy using ion concentrations. To solve for CMIX, the concentration that would result from complete mixing of both streams, we used the following equation:[38,68] The theoretical exergy flow rate from the complete mixing of 3 M ammonia lean and rich solutions at the flow rate used in this work (7.6 mL min–1 cell–1), calculated using eqs and 8, would be approximately 1.24 W, which corresponds to 9800 J L–1 of rich solution or 74 000 J kg–1 of CO2. When we used 3 M ammonia as the lean solution, we measured that we harvested approximately 22 J L–1 of rich solution, which corresponds to 170 J kg–1 of CO2. The CCRED device in this work harvested approximately 0.22% of the theoretical energy that would have resulted from complete mixing of the solutions (Supporting Information). Because we focused on optimizing power density, we harvested a relatively small amount of the theoretical energy that would have been available if more mixing occurred by using slower flow rates, for example. Although we suspect that relatively little mixing occurred within the device,[23] without knowing the ionic concentrations in the effluent, it is impossible to solve for the consumed exergy and energy efficiency. As discussed in previous work, by using the lean solution in the low-salinity compartments, the CCRED system presented in this work likely suffered from a counterproductive hydroxide gradient.[38] The use of nonaqueous amine solvents for carbon capture could eliminate this negative effect caused by hydroxide ions.[71−73] It can be noted that traditional RED systems often achieve energy efficiencies in the range of 20%–40%.[10,14,15,21,66]

Outlook

By using the lean CC solution as the low-salinity solution in a flow-through CCRED system, we improved the feasibility of this technology for integration into existing CC systems. We suggest that the heat exchanger, which already circulates the lean and rich solutions in close contact, potentially provides an opportunity for the seamless incorporation of RED into existing CC infrastructure. Additionally, because the electric potential provided by a RED system increases with temperature (Supporting Information), the heat from the stripping process as well as from the exothermic reaction of CO2 with an amine solvent may enhance the power density of CCRED implemented in industrial settings compared to this laboratory demonstration with room-temperature solutions.[74] Comparing various CC solvents, we achieved the highest power density, 0.94 W m–2, using ammonia. This power density is within the range of reported values for RED systems using ammonium bicarbonate.[46,49,65] Besides the value in electrical power that might be generated using CCRED with ammonia, ammonia solutions can also be regenerated at a lower temperature than any of the other CC solvents considered in this work, possibly only requiring the low-grade waste heat of industrial processes.[29,45,48,49] Further improvements, including the use of thinner compartments or faster flow rates, may be used to increase the power density of CCRED. Especially, the development of ion-selective membranes specific to the CC solvents used could greatly improve the performance of CCRED.[23,57,62,63] Ultimately, this work demonstrated and examined the power output of CCRED using a variety of commonly used CC solvents to encourage further investigation of CCRED as a means of reducing the energetic costs of CC.
  19 in total

1.  Thermodynamic and energy efficiency analysis of power generation from natural salinity gradients by pressure retarded osmosis.

Authors:  Ngai Yin Yip; Menachem Elimelech
Journal:  Environ Sci Technol       Date:  2012-04-13       Impact factor: 9.028

2.  Climate change. Global warming is changing the world.

Authors:  Richard A Kerr
Journal:  Science       Date:  2007-04-13       Impact factor: 47.728

3.  Thermodynamic, energy efficiency, and power density analysis of reverse electrodialysis power generation with natural salinity gradients.

Authors:  Ngai Yin Yip; David A Vermaas; Kitty Nijmeijer; Menachem Elimelech
Journal:  Environ Sci Technol       Date:  2014-04-17       Impact factor: 9.028

4.  Cutting the cost of carbon capture: a case for carbon capture and utilization.

Authors:  Lennart Joos; Johanna M Huck; Veronique Van Speybroeck; Berend Smit
Journal:  Faraday Discuss       Date:  2016-10-20       Impact factor: 4.008

5.  An electric-eel-inspired soft power source from stacked hydrogels.

Authors:  Thomas B H Schroeder; Anirvan Guha; Aaron Lamoureux; Gloria VanRenterghem; David Sept; Max Shtein; Jerry Yang; Michael Mayer
Journal:  Nature       Date:  2017-12-13       Impact factor: 49.962

6.  Carbon dioxide capture: prospects for new materials.

Authors:  Deanna M D'Alessandro; Berend Smit; Jeffrey R Long
Journal:  Angew Chem Int Ed Engl       Date:  2010-08-16       Impact factor: 15.336

7.  Ammonium Bicarbonate Transport in Anion Exchange Membranes for Salinity Gradient Energy.

Authors:  Geoffrey M Geise; Michael A Hickner; Bruce E Logan
Journal:  ACS Macro Lett       Date:  2013-08-22       Impact factor: 6.903

8.  Ionic resistance and permselectivity tradeoffs in anion exchange membranes.

Authors:  Geoffrey M Geise; Michael A Hickner; Bruce E Logan
Journal:  ACS Appl Mater Interfaces       Date:  2013-10-01       Impact factor: 9.229

9.  Powering Electronic Devices from Salt Gradients in AA-Battery-Sized Stacks of Hydrogel-Infused Paper.

Authors:  Anirvan Guha; Trevor J Kalkus; Thomas B H Schroeder; Oliver G Willis; Chris Rader; Alessandro Ianiro; Michael Mayer
Journal:  Adv Mater       Date:  2021-06-24       Impact factor: 30.849

10.  Upscaling Reverse Electrodialysis.

Authors:  Jordi Moreno; Simon Grasman; Ronny van Engelen; Kitty Nijmeijer
Journal:  Environ Sci Technol       Date:  2018-08-27       Impact factor: 9.028

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